Science - 21 October 2011
Science - 21 October 2011
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CONTENTS Volume 334   Issue 6054
pages 315 & 389
page 304
EDITORIAL
289  The Cost of Doing Nothing
Kathy Caldwell
NEWS OF THE WEEK
294   A roundup of the weeks top stories
NEWS & ANALYSIS
298   Vaccine Trial Meets Modest 
Expectations, Buoys Hopes
299   Drug-Screening Program 
Looking for a Home
300  Navy Dives Into Program Offering 
Cash for Good Scores
301   China Looks to Purge Academia 
of Trash Journals
302  Pre-Clovis Mastodon Hunters 
Make a Point
>> Report p. 351
303   In Northern Aral Sea, Rebound Comes 
With a Big Catch
NEWS FOCUS 
304   The Sterile Neutrino: 
Fertile Concept or Dead End?
>> Science Podcast
307   Social Science for Pennies
308  Open-Source Ecology Takes Root 
Across the World
LETTERS
310   Editorial Expression of Concern
B. Alberts
    Martial Arts Research: Prudent Skepticism
J. M. Strayhorn and J. C. Strayhorn
    Martial Arts Research: Weak Evidence
J. Mercer
    Response
A. Diamond and K. Lee
311   CORRECTIONS AND CLARIFICATIONS
311   TECHNICAL COMMENT ABSTRACTS
BOOKS ET AL.
312   Sybil Exposed
D. Nathan, reviewed by B. Harris
EDUCATION FORUM
313   Rethink Summer Student Research
F. A. Carrero-Martnez
PERSPECTIVES
315   The Strength of Electrical Synapses
S. Hestrin
>> Report p. 389
316     Watery Disks
R. Akeson
>> Report p. 338
317     Antenna-Guided Light
N. Engheta
>> Research Article p. 333
318     Eddies Masquerade as Planetary Waves
D. J. McGillicuddy Jr.
>> Research Article p. 328
320     Up Close with Membrane 
Lipid-Protein Complexes
J. Whitelegge
>> Report p. 380
321     Every Bit Counts
P. J. Thomas
>> Report p. 354
REVIEW
323   Globalization, Land Use, and the 
Invasion of West Nile Virus
A. M. Kilpatrick
>> Science Podcast
CONTENTS continued >>
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  281
COVER
 Illustration of a generalized form of Snells Law that fully accounts 
for light interaction with subwavelength structured materials, 
which can produce phase jumps at the interface between media. 
To illustrate this effect, origami ribbons are folded into tapered 
cylinders (phase jumps at interfaces), and the lines (light rays) 
form angles that depend on the degree of taper. Initially diverging 
rays converge after passing through two interfaces. See page 333.
Image: Nanfang Yu/Harvard University; Yi Tan and Jinhua Tan
DEPARTMENTS
285  This Week in Science
290  Editors Choice
292  Science Staff
395  New Products
396  Science Careers
CONTENTS
pages 320 & 380
page 373
page 328
RESEARCH ARTICLES
328   The Inuence of Nonlinear Mesoscale 
Eddies on Near-Surface Oceanic 
Chlorophyll
D. B. Chelton et al.
Large ocean eddies are the cause of some 
sea-surface height and chlorophyll anomalies 
previously ascribed to Rossby waves.
>> Perspective p. 318
333    Light Propagation with Phase 
Discontinuities: Generalized Laws 
of Reection and Refraction
N. Yu et al.
Light propagation can be controlled with 
plasmonic interfaces that introduce abrupt 
phase shifts along the optical path.
>> Perspective p. 317
REPORTS
338   Detection of the Water Reservoir 
in a Forming Planetary System
M. R. Hogerheijde et al.
The detection of cold water vapor in a 
nearby planet-forming disk suggests that 
water ice exists in its outer regions. 
>> Perspective p. 316
340     Supramolecular Linear Heterojunction 
Composed of Graphite-Like Semiconducting 
Nanotubular Segments
W. Zhang et al.
 A supramolecular self-assembly approach is 
used to make a nanotubular heterojunction.
343   Dynamics of the Reaction of Methane 
with Chlorine Atom on an Accurate 
Potential Energy Surface
G. Czak and J. M. Bowman
Theory helps explain the counterintuitive 
impacts of vibrational excitation in a widely 
studied reaction.
347   800,000 Years of Abrupt Climate 
Variability
S. Barker et al.
Greenland climate variability for the 
past 800,000 years was inferred from 
the Antarctic ice-core temperature record.
351   Pre-Clovis Mastodon Hunting 
13,800 Years Ago at the 
Manis Site, Washington
M. R. Waters et al.
Further dating of the Manis site shows 
that people were hunting mastodons in 
North America by 14,000 years ago.
>> News story p. 302; Science Podcast
354   Information Transduction Capacity of 
Noisy Biochemical Signaling Networks
R. Cheong et al.
Noise limits information transfer through 
a single signaling pathway in a single cell 
to just one bit.
>> Perspective p. 321
358   ER Tubules Mark Sites of 
Mitochondrial Division
J. R. Friedman et al.
Mitochondrial division occurs at positions 
where endoplasmic reticulum tubules contact 
mitochondria and mediate constriction.
362   Antimicrobial Peptides Keep Insect 
Endosymbionts Under Control
F. H. Login et al.
A beetle species synthesizes an antimicrobial 
peptide to constrain a bacterial symbiont in 
specialized organs.
366     Stochastic Pulse Regulation in 
Bacterial Stress Response
J. C. W. Locke et al.
Energy stress activates an alternative sigma 
factor in stochastic pulses and modulates 
pulse frequency to control activity.
369     Transgenerational Epigenetic Instability 
Is a Source of Novel Methylation Variants
R. J. Schmitz et al.
Spontaneous methylation rates that may 
affect phenotype in the plant Arabidopsis 
are higher than the mutation rate. 
373     Computation-Guided Backbone Grafting 
of a Discontinuous Motif onto a Protein 
Scaffold
M. L. Azoitei et al.
A two-segment HIV epitope grafted into 
a scaffold protein maintains high afnity 
for a broadly neutralizing antibody.
376   Antagonists Induce a Conformational 
Change in cIAP1 That Promotes 
Autoubiquitination
E. C. Dueber et al.
Antagonist binding to an apoptosis inhibitor 
releases inhibition by promoting dimerization 
required for autoubiquitination.
380   Mass Spectrometry of Intact V-Type 
ATPases Reveals Bound Lipids and the 
Effects of Nucleotide Binding
M. Zhou et al.
The effect of lipids and nucleotides on 
the soluble head domain and membrane 
base domain is examined in an intact 
adenosine triphosphatase.
>> Perspective p. 320
385   Cerebellum Shapes Hippocampal 
Spatial Code
C. Rochefort et al.
Cerebellar protein kinase Cdependent 
mechanisms process self-motion information 
needed for spatial representation and 
accurate navigation.
389     Activity-Dependent Long-Term Depression 
of Electrical Synapses
J. S. Haas et al.
Paired bursting in coupled neurons depresses 
electrical synapses while their asymmetry 
increases after unidirectional use.
>> Perspective p. 315
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  282
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  283
CONTENTS
SCIENCEXPRESS
www.sciencexpress.org
Structural Dynamics of a Catalytic Monolayer 
Probed by Ultrafast 2D IR Vibrational Echoes
D. E. Rosenfeld et al.
A method to track fast vibrational motion in 
solution has been extended to catalytically 
important solid/liquid interfaces.
10.1126/science.1211350
Wolbachia Enhance Drosophila Stem Cell 
Proliferation and Target the Germline 
Stem Cell Niche
E. M. Fast et al.
A bacterial endosymbiont up-regulates mitosis 
of Drosophila germline stem cells and blocks 
programmed cell death.
10.1126/science.1209609
Endocannabinoid Hydrolysis Generates Brain 
Prostaglandins That Promote Neuroinammation
D. K. Nomura et al.
A new tissue-specic pathway for the synthesis 
of proinammatory prostaglandins is described.  
10.1126/science.1209200
Recent Synchronous Radiation of a Living Fossil 
N. S. Nagalingum et al.
Despite their ancient origin, the majority of
extant cycad species radiated within the past 
10 million years.
10.1126/science.1209926
Polarization of PAR Proteins by Advective 
Triggering of a Pattern-Forming System 
N. W. Goehring et al.
Patterning of Caenorhabditis elegans zygotes 
involves passive as well as active mechanisms.
10.1126/science.1208619
TECHNICALCOMMENTS
Comment on How Cats Lap: Water Uptake 
by Felis catus
M. Nauenberg
Full text at www.sciencemag.org/cgi/content/
full/334/6054/311-b
Response to Comment on How Cats Lap: 
Water Uptake by Felis catus
R. Stocker et al.
Full text at www.sciencemag.org/cgi/content/
full/334/6054/311-c
SCIENCENOW
www.sciencenow.org  
Highlights From Our Daily News Coverage
Cute TV Chimps May Harm Their Wild Brethren
Seeing dressed-up chimpanzees doesnt make 
viewers care more.
http://scim.ag/chimpads
Seaweed With a Deadly Touch 
Toxins on the surfaces of common South Pacic 
algae are deadly to corals.
http://scim.ag/CSlamphora
Winged Robots Hint at the Origins of Flight
What were primitive wings used for before 
bird ancestors could y?
http://scim.ag/robot-ight
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SCIENCESIGNALING 
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18 October issue: http://scim.ag/ss101811
RESEARCH ARTICLE: Agrobacterium 
Counteracts Host-Induced Degradation 
of Its Effector F-Box Protein
S. Magori and V. Citovsky
A plant pathogen prevents degradation of its key 
virulence factor in infected host cells.
REVIEW: Structural Basis for Activation and 
Inhibition of Class I Phosphoinositide 3-Kinases
O. Vadas et al.
The regulatory interactions between PI3Ks and their 
binding partners could be exploited for therapies.
JOURNAL CLUB: -Synuclein Promotes 
Neuroprotection Through NF-BMediated 
Transcriptional Regulation of Protein Kinase C
R. Aoki and Y. R. Li 
-Synuclein may protect dopaminergic neurons 
from apoptosis by reducing the abundance 
of a kinase involved in cell death.
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Integrating Medicine and Science
19 October issue: http://scim.ag/stm101911
 FOCUS: Containing the Contagion 
Treating the Virus That Inspired the Film
B. Lee
RESEARCH ARTICLE: A Neutralizing Human 
Monoclonal Antibody Protects African Green 
Monkeys from Hendra Virus Challenge 
K. N. Bossart et al.
A neutralizing human monoclonal antibody 
can fully protect nonhuman primates from 
disease after a lethal Hendra virus challenge.
PERSPECTIVE: Hedgehog Rushes to the 
Rescue of the Developing Cerebellum
O. Baud and P. Gressens
RESEARCH ARTICLE: A Small-Molecule 
Smoothened Agonist Prevents Glucocorticoid-
Induced Neonatal Cerebellar Injury
V. M. Heine et al.
RESEARCH ARTICLE: Preterm Cerebellar Growth 
Impairment After Postnatal Exposure to 
Glucocorticoids
E. W. Y. Tam et al.
A small molecule that targets the sonic hedgehog 
pathway protects against cerebellar injury caused 
by glucocorticoids, which may be given to preterm 
infants for treating lung disease.
SCIENCECAREERS
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Tooling Up: Views on an Interview, Part 1
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 Scott Jacksons interview at ABC technologies 
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D. Albert
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to employ indirect means.
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 Content Collection: Careers at Nonprots
E. Pain
Scientists interested in a social or humanitarian cause 
can nd diverse research or alternative careers within 
nonprot organizations.
http://scim.ag/CC_Nonprots
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On the 21 October Science Podcast: mastodon 
hunting before Clovis, globalization and West Nile 
virus, the search for the sterile neutrino, and more.
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www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011
Virus Invasion
West Nile virus is spread through mosquitoes to 
birds, wildlife, and humans and has established 
itself at an astonishingly rapid rate since it was 
introduced to North America in 1999. How did 
the West Nile virus establish itself so successfully 
to the detriment of human and wildlife popula-
tions? Kilpatrick (p. 323) reviews the scenarios 
and dynamics that point to the key bird hosts 
and the relative predilections of the associated 
mosquito vectors to feed on a variety of animals, 
including humans. 
Making Waves
Patterns of ocean chlorophyll variability from 
satellite observations have been attributed to oce-
anic Rossby wavesslow-moving features with 
wavelengths of hundreds of kilometers but with 
sea surface heights of only centimetersthat 
take months or years to cross ocean basins from 
the west to the east. Chelton et al. (p. 328, pub-
lished online 15 September; see the Perspective 
by McGillicuddy) report that the cause of these 
chlorophyll anomalies has been misidentied. 
Analysis of 10 years of remotely observed sea sur-
face height elds and concurrent observations of 
upper-ocean chlorophyll concentrations suggests 
that the dominant mechanism controlling the 
development of these anomalies is the horizontal 
advection of chlorophyll-rich surface water caused 
by the rotational motions of eddies.
Nano-Heterojunction 
Self-Assembly
Nanoscale materials can now be syn-
thesized by a wide range of methods, 
including self-assembly techniques. 
The junction regions between dissimilar materials 
often have unusual and desirable properties. 
Zhang et al. (p. 340) were able to extend the 
self-assembly toolbox to make heterojunctions of 
semiconducting nanotubular segments. The con-
joined segments could transport electrical charge 
and also increase the lifetime of photogenerated 
charge carriers.
Controlling Light 
The behavior of light as it propagates through a 
material and from one material to another is very 
well understood in terms of classical optics. Yu et 
al. (p. 333, published online 1 September; see the 
cover; see the Perspective by Engheta) now dem-
onstrate a powerful new method to control light 
propagation, based on introducing abrupt phase 
shifts along the optical path. These phase disconti-
nuities are constructed using plasmonic interfaces 
that consist of an optically thin two-dimensional 
matrix of optical antennas with subwavelength 
separation. The exibility of the technique should 
prove useful for developing a wide variety of 
small-footprint planar optical components.
Whence the Water Vapor?
Water vapor has been detected in the inner regions 
of planet-forming diskswhere terrestrial planets 
are created. Using the Heterodyne Instrument 
for the Far-Infrared on board the Herschel Space 
Observatory, Hogerheijde et al. (p. 338; see the 
Perspective by Akeson) now report the detection of 
water vapor over the full extent of the disk around 
the young star TW Hydrae. In the outer regions of 
this planet-forming disk, water vapor could only 
originate from icy grains. Thus, the result suggests 
the presence of a large reservoir of water ice in the 
region where comets and giant planets form.
When Cl and CH
4
 Collide
The simplest class of two-body chemical reaction 
is the formation of a diatomic molecule. Two 
atoms come together and, generally speaking, 
the only variable is their relative velocity. Things 
get considerably more complicated if you add 
another atom to the mix and consider its reaction 
with a preformed diatomic. Now, there are rela-
tive spatial orientations, and the diatomic might 
be vibrating or rotating. Nonetheless, over the 
past half-century or so, chemists have developed 
a rm grasp of how these reactions work in detail. 
The next frontier will be to understand how an 
atom reacts with a polyatomic, which has many 
different ways of vibrating. Czak and Bowman 
(p. 343) simulated the reactivity of methane with 
a chlorine atom, providing a theoretical basis for 
a multitude of pivotal experiments on this system.
Polar Connections 
The climate records extracted from ice cores re-
covered from the Greenland Ice Sheet are detailed 
but relatively short in durationaround 120,000 
years. Ice cores from Antarctica, on the other 
hand, have lower temporal resolution but extend 
back more than 800,000 years. In order to infer 
how Greenlands climate may have varied over a 
longer interval, Barker et al. (p. 347, published 
online 8 September) used the Antarctic tempera-
ture record, data from Chinese speleothems, and 
the concept of the bipolar seesaw to produce a 
well-dated reconstruction of inferred Greenland 
temperature variability. Abrupt shifts in Northern 
Hemisphere climate appear to have occurred 
throughout the Late Pleistocene, and glacial 
terminations may have been linked to oscillations 
of the bipolar seesaw. 
Control and Cooperation 
How do hosts regulate internal symbionts to prevent them from taking over their bodies without 
compromising  the  advantages  of  the  relationship?  Login  et  al.  (p.  362)  explored  the  balance 
between host innate immune responses and bacterial replication of an endosymbiont in weevils, 
an  important  beetle  pest  of  wheat. A  single  peptide,  coleoptericin-A  (ColA),  synthesized  by  the 
beetle constrained the bacteria within bacteriocytes and blocked bacterial replication. When the 
weevils  ColA  expression  was  silenced,  the  bacteria  were  able  to  replicate  normally,  escape  the 
bacteriocyte, and spread throughout the insect.
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 This Week in Science
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Hunting Mastodons
A mastodon skeleton containing an embedded projectile tip was discovered in the late 1970s near 
Manis, Washington. It was initially dated as about 14,000 years ago but the age, and whether the bone 
containing the projectile was directly associated with the rest of the skeleton, has been questioned. 
Waters et al. (p. 351) provide new dates on the fossils that conrm an age of about 14,000 years ago. 
The data, together with genetic analyses, show that the skeletal elements are related and also that the 
projectile was fashioned from a mastodon bone. This age predates the Clovis culture in North America 
and, along with other sites, shows early exploitation of megafauna.
Tumor Necrosis Factor Response
Engineers use information theory to analyze how noise inuences information transfer, for example, 
in telephone systems. Cheong et al. (p. 354, published online 15 September; see the Perspective 
by Thomas) have now applied such analysis in biological experiments by monitoring the response 
of thousands of single mouse broblasts to stimulation with various doses of tumor necrosis factor 
(TNF). Signal transmission was surprisingly noisy, meaning that the cells could only really differ-
entiate whether TNF was present or not. Such limitations of a single signaling pathway appear to 
be overcome by the cooperation of multiple signaling pathways in networks, or by groups of cells 
collectively averaging their response to the same signal.
Mitochondrial Division 
Mitochondrial division regulates both the shape and the distribution of the mitochondrial 
network, which is important in maintaining cellular health. Friedman et al. (p. 358, pub-
lished online 1 September; see the 14 October Perspective by Rambold and Lippincott-
Schwartz) demonstrate that mitochondria in both yeast and mammalian cells are constricted 
and divide at positions where they form stable contact sites with the endoplasmic reticulum. 
Not in the Genes
The mechanism, distribution, and function of DNA methylation in plant genomes have been char-
acterized, but the stability of DNA methylation over multiple generations and the rate of change 
are less well understood. Schmitz et al. (p. 369, published online 15 September) determined the 
methylation status of several previously sequenced Arabidopsis lines, including three ancestral and 
ve descendant lines separated by 30 generations. The frequency of DNA methylation changes was 
5 orders of magnitude higher than genetic changes. Also, unlike genetic changes that were mostly 
random, DNA methylation changes occurred in hotspots.
Improving the Fit
Designing proteins for specic functions often relies on grafting functional groups onto existing 
protein scaffolds. Success has been limited because backbone remodeling, which might allow more 
complex grafting, has been computationally challenging. Azoitei et al. (p. 373) integrated com-
putational design and directed evolution to enable the manipulation of protein backbone structure 
required for transplantation of the backbone and side chains of discontinous functional motifs. They 
grafted a two-segment HIV gp120 epitope that is targeted by the cross-neutralizing antibody b12, 
onto an unrelated scaffold. The nal design showed high afnity and specicity for b12 and the 
complex structurally mimicked the gp120-b12 interaction.
Navigating with the Cerebellum
To navigate in space, animals use two strategies: landmark-assisted or map-navigation, which requires 
self-motion cues. Although the cerebellum is known to assist in the coordination of self-motion informa-
tion, its role in spatial navigation is unclear. Rochefort et al. (p. 385) examined whether impairment 
of the cerebellum affects the spatial code in the hippocampus, using transgenic mice with a selective 
disruption of protein kinase Cdependent plasticity at parallel berPurkinje cells synapses. Although 
landmark-assisted navigation was robust, when the mice had to rely on motion-generated cuesfor 
example, in the darknavigation suffered. 
Continued from page 285
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Few, if any, proteins carry out their function in isolation. More likely is that they interact with one or more other proteins, during 
which conformational changes and even physical modications such as phosphorylation may occur. The ability to detect both 
the  interaction  and  modication  of  proteins  is  critical  to  elucidating  function  and  dysfunction  in  cells  and  tissues,  leading 
to a deeper understanding of normal as well as diseased states. This webinar will focus on current methodologies available 
to  study  protein-protein  interactions,  as  well  as  looking  at  new  technologies  for  characterizing  protein  binding  events  in  a 
noninvasive manner that more closely resembles a cells natural environment, producing more physiologically relevant data. 
During the webinar, our expert panelists will:
  Explain how protein structure and function can be affected by 
posttranslational modications and interactions with diverse partners
  Discuss current state-of-the-art methods and technologies for 
characterizing protein-protein interactions and modications
  Describe how multiplexing can be used to distinguish similar 
biomolecular events, such as multiphosphorylated molecules or 
multiple interacting partners
  Answer your questions live and in real time!
Webinar sponsored by 
Brought  to you by the 
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Participating Experts
Anton Simeonov, Ph.D.
National Institutes of Health
Bethesda, MD
James Bradner, M.D.
Dana-Farber Cancer Institute
Boston, MA
Mathieu Arcand, Ph.D.
PerkinElmer
Montral, Canada
Detecting Native 
Protein Interaction 
and Phosphorylation
New Approaches and 
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WEBINAR
November 9, 2011
12 noon Eastern, 9 a.m. Pacic, 5 p.m. GMT
 The Cost of Doing Nothing 
AS  THE  U.S.  CONGRESS  GRAPPLES  FOR  SOLUTIONS  TO  THE  ECONOMIC  CRISIS,  IT  IS  CRITICAL 
to recognize that rebuilding and modernizing infrastructure will be a key driver of economic 
growth. Recent reports issued by the American Society of Civil Engineers (ASCE),* the 
Urban Land Institute,  and Building Americas Future have described the deterioration 
of the nations energy, water, and transportation infrastructure. This week, ASCE convenes 
its annual meeting, gathering international scientists, engineers, policy-makers, and educa-
tors to share sustainable solutions across a broad spectrum of concerns in the natural and 
built environment. Key among the discussions will be the role of scientists and engineers 
in developing effective public policy, helping to produce an infrastructure that incorporates 
new materials, technologies, and strategies to improve environmental and social well-being. 
When the ASCE issued its 2009 Report Card for Americas Infrastructure, it gave the 
cumulative grade of D to the condition and performance of 15 of 
the countrys infrastructure systems.* Among the worst were roads 
and drinking water. The United States not only loses about seven bil-
lion gallons of clean drinking water every day due to leaking water 
systems, but pipe failures and resulting oods have collapsed roads, 
destroyed homes, and endangered people. It would require an esti-
mated $2.2 trillion over 5 years to raise the grade for all 15 infra-
structure systems to an acceptable level. Sadly, the situation has not 
changed since the report was published. Earlier this year, the ASCEs 
report Failure to Act, The Economic Impact of Current Investment 
Trends in Surface Transportation Infrastructure determined that the 
decient surface transportation infrastructure alone will cost U.S. 
businesses an added $430 billion (cumulative to 2020) in transpor-
tation costs. By 2020, it is projected that exports will be $28 billion 
lower, 70,000 jobs will be lost, households will lose more than $7000 
in personal income, and the countrys gross domestic product will take a hit of $897 billion. 
Businesses will need to divert increasing portions of income to pay for transportation delays, 
wasting money that could instead be invested in innovation. Nearly all sectors will suffer, but 
those associated with technology and innovation would probably be the hardest hit. 
To meet the many infrastructure challenges, more nancing is needed. Now that the 
American Jobs Act has failed to pass Congress, there is discussion of breaking the bill into 
pieces that should be easier to pass. The proposed act includes $50 billion to modernize road, 
rail, and air transportation systems, and it would establish a National Infrastructure Bank to 
leverage public and private capital toward these endeavors. This level of priority and invest-
ment is needed, or the United States will continue its downward slide. Indeed, this years 
report from the Urban Land Institute warns that the United States has fallen behind Brazil, 
China, and India in bolstering transportation, water, and sewage infrastructure.  
Promoting a more sustainable and resilient infrastructure must also be part of this con-
versation. Improved design and construction standards to withstand extreme conditions will 
require further R&D. Climate change and environmental preservation also require innova-
tive infrastructure designs. Research is needed to determine the best ways to expand power 
generation and transmission. And the growing demands for information technology mean 
that underground utilities must be carefully planned. 
Infrastructure investments provide an opportunity to improve the economy in the short term 
by creating jobs, while also driving the long-term growth needed to compete in the global mar-
ketplace. Although repairing and modernizing the countrys infrastructure may seem daunting 
in lean times, the cost of doing nothing will be exponentially greater. 
10.1126/science.1214039
 Kathy Caldwell 
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Civil Engineers. E-mail: 
kcaldwell@asce.org. 
www.sciencemag.org    SCIENCE    VOL 334   21 OCTOBER 2011 
*www.asce.org/reportcard.   www.uli.org/~/media/Documents/ResearchAndPublications/Reports/Infrastructure/
Infrastructure2011.ashx.  www.bafuture.org/report.  www.asce.org/uploadedFiles/Infrastructure/Report_Card/
ASCE-FailureToActFinal.pdf.   
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EDITED BY KRISTEN MUELLER AND JAKE YESTON
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21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org 
O C E A N   S C I E N C E
What Keeps the Storms Away?
The number of hurricanes that develop over the 
Atlantic Ocean each year and the number that 
make landfall in North and Central America are 
two distinct quantities. The difference between 
the two has great practical consequence, as 
hurricanes that remain offshore cause few 
deaths and do little damage to human prop-
erty or infrastructure. What controls hurricane 
tracks, then? Wang et al. looked at sea surface 
temperature data from 1970 to 2009 and found 
that the size and location of the Atlantic warm 
pool help to steer hurricanes by inuencing 
both where over the Atlantic they form and to 
what extent ensuing atmospheric circulation 
patterns push the storms away from the eastern 
seaboard of the United States. When the Atlantic 
warm pool is large, storms form more to the 
east, further from potential landfall, and the 
winds along their paths blow more strongly 
toward the northeast, also reducing the chance 
that the storms ultimately reach a vulnerable 
coast. Although these are not the only factors 
that control hurricane tracks, consideration of 
the sea surface temperature elds of the North 
Atlantic Ocean may help improve forecasts of 
potential hurricane dangers.  HJS
Geophys. Res. Lett. 38, L19702 (2011).
P L A N E T A R Y   S C I E N C E
Why No Clay Up North?
The surface of Mars can be divided into two 
major regions: the northern lowlands and the 
southern highlands. The lowlands, covering 
around 1/3 of the planet, are thought to have 
once been the site of an ancient, great northern 
ocean. However, this hypothesis 
is at odds with the record 
of the presence of 
clay deposits. These 
sediments, whose 
formation requires 
the presence of 
liquid water, 
are widespread 
in the southern 
highlands but very 
scarcely distributed 
in the northern low-
lands. Using a climate 
model, Fairn et al. deter-
mined the surface temperatures 
on early Mars, assuming a southern super-
continent and a northern ocean. The model tem-
peratures imply that the northern ocean would 
H Y D R O L O G Y
Rolling Down the River
All rivers naturally move loads of sediments, 
from coarse sand grains rolling along river-
beds to tiny clay and silt particles carried in 
suspension. When sediment load gets too 
high though, either naturally or from hu-
man activities, biodiversity suffers and water 
quality deteriorates. Identifying the sources of 
increased sediment loads, which can vary with 
such regional factors as land use and precipita-
have had to be a glacial ocean similar to the 
seas in Earths polar regions. Calculations of the 
rate of clay formation at subzero temperatures 
support the lack of clays in the northern low-
lands, because their formation would have been 
inhibited at those cold temperatures. Moreover, 
the presence of glaciers surrounding the north-
ern ocean would have limited the transport of 
continental sediments into the ocean, as is the 
case in the Arctic and Antarctic coastal regions 
of Earth.  MJC
Nat. Geosci. 4, 667 (2011).
E C O N O MI C S
Resource Investment
As Newton famously noted, researchers stand on the shoulders of giants, building on accu-
mulated knowledge. But the mere production of knowledge does not ensure its use by others; 
societal benet depends also on mechanisms for storing and accessing knowledge. Research-
ers have sought to understand how different institutions and policies can promote knowledge 
use and impact. To explore impacts of institutional resources in the life sciences, Furman and 
Stern studied the American Type Culture Collection (ATCC). Among the worlds largest bio re-
source centers, ATCC maintains and distributes a vast collection of cell lines and microbiology 
cultures.  Because  each  specimen  deposited  in ATCC  is  accompanied  by  an  initial  character-
ization in a journal article, bibliometric analyses of article citations provided tools to assess 
impacts of ATCC. Besides comparing articles that did and did not link to ATCC specimens, the 
authors also analyzed the timing of citation boosts, because the deposition of specimens at 
ATCC often did not occur until sometime after the initial journal article describing the speci-
men. The ATCC-deposit citation boost ranged from 57 to 135%, was higher for articles in less 
prestigious journals, and was concentrated on follow-up research into more complex subject 
matter. A rough approximation of cost per citation suggested that funders might consider 
increased investments in ensuring access to existing research rather than focusing so much 
on new research.  BW
Am. Econ. Rev. 101, 1933 (2011). 
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www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011
tion, is critical for implementing remediation 
strategies. As a case study for determining the 
mechanism of sediment transport on the scale of 
several watersheds, Belmont et al. integrated a 
number of data sourcesincluding geochemi-
cal tracers, hydrologic eld measurements, and 
remote sensingfrom tributaries or lakes in 
Minnesota along North Americas largest river, 
the Mississippi. Over the past 150 years, not 
only has the amount of ne-grained sediment 
increased by a factor of 10, but the sources have 
also changed. Historically, upland erosion of soil 
contributed most of the sediment load; however, 
the new data suggest that up to 70% of the 
sediment comes from the erosion of riverbanks 
and ravines themselves. The shift is probably 
a function of both natural and anthropogenic 
activity, including increased precipitation and 
extensive modication of drainage networks for 
agricultural purposes.  NW 
Environ. Sci. Technol. 45, 10.1021/es2019109 
(2011).
MI C R O B I O L O G Y
Rapid Transport
E-cadherin is a species-specic receptor for the 
foodborne pathogen Listeria monocytogenes 
but it is located out of reach beneath the tight 
junctions formed between gut epithelial cells. 
Does the dynamic nature of the intestinal epi-
thelium, which is being remodeled constantly, 
with cells being shed and mucus secreted, 
allow for E-cadherin to be accessed? Taking a 
step back from molecu-
lar studies of pathogen 
cell invasion, Nikitas et 
al. watched how Listeria 
invades the body, using 
humanized mice and 
two-photon and confocal 
microscopy. They found 
that E-cadherin is not 
perpetually out of sight 
but becomes exposed 
to the intestinal lumen 
when cells are extruded 
and cell junctions are disrupted by contracting 
goblet cells or folds in the villi. Once inside the 
cell, the bacteria have no need for any other 
virulence factors, neither listeriolysin-O nor ActA 
(which polymerizes the cells actin). All that is 
required is the bacterial surface protein InlA 
for rapid apico-basal translocation mediated by 
the cells microtubules and exocytosis into the 
lamina propria. Thirty minutes after invasion, 
and Listeria had entered the spleen undetected 
by immune surveillance and a systemic infection 
was established.  CA
J. Exp.Med. 208, 10.1084/jem.20110560 (2011).
P S Y C H O L O G Y
Thats Not Yours!
Much ink has been spilled in arguments about 
what it is that children have learned when 
they begin to grasp the possibility that other 
peoples beliefs can differ from their own. But 
what do children comprehend of other peoples 
rights, such as the ownership of property? 
Rossano et al. describe experimental results 
indicating that 3-year-old children exhibit a 
more sophisticated understanding of the rights 
conferred by ownershipin this instance, the 
disposal of a cap or scarfthan 2-year-olds. 
Children of both ages complained when their 
own hat was thrown away by a puppet, and they 
did not protest when the puppet threw away his 
own article of clothing; the key distinction was 
that older kids registered a normative objection 
when the puppet discarded a hat belonging 
to a third party (the experimenter). In their 
introduction to an edited collection, Friedman 
and Ross enumerate the reasons why research 
on the developmental origins of ownership will 
yield ndings of interest.  GJC
Cognition 121, 219 (2011); New Dir. Child Ado-
lesc. Dev. 132, 1 (2011).
C E L L   S I G N A L I N G
Enlightening the Load
If you have driven a car with a manual transmis-
sion, you are aware that the response to the 
throttle is quite different when the drive train is 
connected to a load (when the 
clutch is engaged and the engine 
drives the wheels) than when it is 
not (when the engine spins freely 
with the clutch disengaged). 
Jiang et al. explored whether a 
similar concept of load applies 
to biochemical signaling systems; 
that is, whether the dynamic 
properties of a signaling mecha-
nism were altered in the presence 
or absence of substrate molecules 
that are targets of the system. 
Combined experiments and mathematical 
modeling showed that the presence of substrate 
could alter the response time of the system, 
increasing it when one of the enzymes in the 
signaling system was operating at a maximal 
rate (saturated) but decreasing it when the
enzymes were operating in a linear manner. The 
authors discuss how such effects of downstream 
targets on the responsiveness of signaling 
systems might be used to design appropriate 
responses when modifying biological systems or 
designing synthetic ones.  LBR
Sci. Sig. 4, ra67 (2011).
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292 21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org 
www.sciencemag.org
SENIOR EDITORIAL BOARD
A. Paul Alivisatos, Lawrence Berkeley Nat'l. Laboratory
Cori Bargmann, The Rockefeller Univ.
Ernst Fehr, Univ. of Zurich
Richard Losick, Harvard Univ.
Michael S. Turner, University of Chicago
BOARD OF REVIEWING EDITORS
Adriano Aguzzi, Univ. Hospital Zrich
Takuzo Aida, Univ. of Tokyo
Sonia Altizer, Univ. of Georgia
Sebastian Amigorena, Institut Curie
Angelika Amon, MIT
Kathryn Anderson, Memorial Sloan-Kettering Cancer Center
Siv G. E. Andersson, Uppsala Univ.
Peter Andolfatto, Princeton Univ.
Meinrat O. Andreae, Max Planck Inst., Mainz
John A. Bargh, Yale Univ.
Ben Barres, Stanford Medical School
Jordi Bascompte, Estacin Biolgica de Doana, CSIC
Facundo Batista, London Research Inst.
Ray H. Baughman, Univ. of Texas, Dallas
David Baum, Univ. of Wisconsin
Yasmine Belkaid, NIAID, NIH 
Philip Benfey, Duke Univ. 
Stephen J. Benkovic, Penn State Univ.
Gregory C. Beroza, Stanford Univ.
Peer Bork, EMBL
Bernard Bourdon, Ecole Normale Superieure de Lyon 
Ian Boyd, Univ. of St. Andrews
Paul M. Brakeeld, Univ. of Cambridge 
Christian Bchel, Universittsklinikum Hamburg-Eppendorf
Joseph A. Burns, Cornell Univ. 
William P. Butz, Population Reference Bureau
Gyorgy Buzsaki, Rutgers Univ.
Mats Carlsson, Univ. of Oslo 
Mildred Cho, Stanford Univ. 
David Clapham, Childrens Hospital, Boston 
David Clary, Univ. of Oxford 
J. M. Claverie, CNRS, Marseille 
Jonathan D. Cohen, Princeton Univ.
Robert Cook-Deegan, Duke Univ. 
Alan Cowman, Walter & Eliza Hall Inst. 
Robert H. Crabtree, Yale Univ.
Wolfgang Cramer, Medit. Inst. for Ecology & Paleoecology
F. Fleming Crim, Univ. of Wisconsin 
Jeff L. Dangl, Univ. of North Carolina
Tom Daniel, Univ. of Washington
Stanislas Dehaene, Collge de France
Emmanouil T. Dermitzakis, Univ. of Geneva Medical School
Robert Desimone, MIT
Claude Desplan, New York Univ.
Ap Dijksterhuis, Radboud Univ. of Nijmegen
Dennis Discher, Univ. of Pennsylvania 
Jennifer A. Doudna, Univ. of California, Berkeley
Julian Downward, Cancer Research UK 
Bruce Dunn, Univ. of California, Los Angeles 
Christopher Dye, WHO
David Ehrhardt, Carnegie Inst. of Washington
Michael B. Elowitz, Calif. Inst. of Technology
Tim Elston, Univ. of North Carolina at Chapel Hill 
Gerhard Ertl, Fritz-Haber-Institut, Berlin 
Barry Everitt, Univ. of Cambridge 
Paul G. Falkowski, Rutgers Univ. 
Ernst Fehr, Univ. of Zurich
Tom Fenchel, Univ. of Copenhagen 
Alain Fischer, INSERM 
Wulfram Gerstner, EPFL Lausanne
Karl-Heinz Glassmeier, TU Braunschweig
Diane Grifn, Johns Hopkins Bloomberg School of 
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Elizabeth Grove, Univ. of Chicago
Taekjip Ha, Univ. of Illinois at Urbana-Champaign
Christian Haass, Ludwig Maximilians Univ.
Steven Hahn, Fred Hutchinson Cancer Research Center
Gregory J. Hannon, Cold Spring Harbor Lab.
Martin Heimann, Max Planck Inst., Jena
Isaac Held, NOAA 
James A. Hendler, Rensselaer Polytechnic Inst.
Janet G. Hering, Swiss Fed. Inst. of Aquatic 
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Ray Hilborn, Univ. of Washington
Michael E. Himmel, National Renewable Energy Lab.
Kai-Uwe Hinrichs, Univ. of Bremen
Kei Hirose, Tokyo Inst. of Technology
David Hodell, Univ. of Cambridge
Ove Hoegh-Guldberg, Univ. of Queensland
David Holden, Imperial College
Lora Hooper, UT Southwestern Medical Ctr at Dallas
Jeffrey A. Hubbell, EPFL Lausanne
Steven Jacobsen, Univ. of California, Los Angeles
Kai Johnsson, EPFL Lausanne
Peter Jonas, Universitt Freiburg
William Kaelin, Dana-Farber Cancer Inst.
Barbara B. Kahn, Harvard Medical School
Daniel Kahne, Harvard Univ.
Bernhard Keimer, Max Planck Inst., Stuttgart
Joel Kingsolver, Univ. of North Carolina at Chapel Hill 
Robert Kingston, Harvard Medical School
Alberto R. Kornblihtt, Univ. of Buenos Aires
Leonid Kruglyak, Princeton Univ.
Mitchell A. Lazar, Univ. of Pennsylvania
David Lazer, Harvard Univ. 
Virginia Lee, Univ. of Pennsylvania
Ottoline Leyser, Cambridge Univ.
Olle Lindvall, Univ. Hospital, Lund
Marcia C. Linn, Univ. of California, Berkeley
John Lis, Cornell Univ.
Jianguo Liu, Michigan State Univ.
Richard Losick, Harvard Univ.
Jonathan Losos, Harvard Univ. 
Ke Lu, Chinese Acad. of Sciences
Laura Machesky, CRUK Beatson Inst. for Cancer Research
Andrew P. MacKenzie, Univ. of St Andrews 
Anne Magurran, Univ. of St Andrews
Oscar Marin, CSIC & Univ. Miguel Hernndez
Charles Marshall, Univ. of California, Berkeley
Martin M. Matzuk, Baylor College of Medicine
Graham Medley, Univ. of Warwick
Yasushi Miyashita, Univ. of Tokyo
Richard Morris, Univ. of Edinburgh
Edvard Moser, Norwegian Univ. of Science and Technology
Sean Munro, MRC Lab. of Molecular Biology
Thomas Murray, The Hastings Center
Naoto Nagaosa, Univ. of Tokyo 
James Nelson, Stanford Univ. School of Med. 
Timothy W. Nilsen, Case Western Reserve Univ. 
Pr Nordlund, Karolinska Inst.
Helga Nowotny, European Research Advisory Board
Luke O'Neill, Trinity College, Dublin
Stuart H. Orkin, Dana-Farber Cancer Inst.
Christine Ortiz, MIT
Elinor Ostrom, Indiana Univ.
Andrew Oswald, Univ. of Warwick
Jane Parker, Max-Planck Inst. of Plant Breeding Research
Donald R. Paul, Univ. of Texas at Austin
P. David Pearson, Univ. of California, Berkeley
Reginald M. Penner, Univ. of California, Irvine
John H. J. Petrini, Memorial Sloan-Kettering Cancer Center
Simon Phillpot, Univ. of Florida 
Philippe Poulin, CNRS 
Colin Renfrew, Univ. of Cambridge
Trevor Robbins, Univ. of Cambridge 
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Jens Rostrup-Nielsen, Haldor Topsoe
Edward M. Rubin, Lawrence Berkeley National Lab
Mike Ryan, Univ. of Texas, Austin
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Miquel Salmeron, Lawrence Berkeley National Lab
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Randy Seeley, Univ. of Cincinnati
Vladimir Shalaev, Purdue Univ.
Joseph Silk, Univ. of Oxford
Denis Simon, Univ. of Oregon
Alison Smith, John Innes Centre 
Davor Solter, Inst. of Medical Biology, Singapore
John Speakman, Univ. of Aberdeen
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Jonathan Sprent, Garvan Inst. of Medical Research
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Bert Vogelstein, Johns Hopkins Univ.
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Ian A. Wilson, The Scripps Res. Inst.
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Jan Zaanen, Leiden Univ.
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EDITOR-IN-CHIEF Bruce Alberts
  EXECUTIVE EDITOR   NEWS EDITOR
  Monica M. Bradford  Colin Norman
MANAGING EDITOR, RESEARCH JOURNALS Katrina L. Kelner
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21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org 294
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Sriharikota on the Bay of Bengal. 
The $125 million mission will study the 
dynamics of cloud formation over the trop-
ics, and how climate change could be affect-
ing the monsoon. As it circles Earth near the 
equator, Megha Tropiques will revisit the 
same regions more than a dozen times each 
day, simultaneously measuring water vapor, 
clouds, precipitation, and radiation. These 
multiple measurements, mission scientists 
say, will give unique insights into the minu-
tiae of how clouds are born 
and die during the 
monsoon. 
India and France have agreed to make 
scientic data from the satellite freely avail-
ablea welcome prospect for atmospheric 
scientists, says Christian Kummerow at 
Colorado State University, Fort Collins. 
It is a very exciting mission and we do 
look forward to receiving the data from 
its instruments.
Indian Ocean  3
Tsunami Warning System Passes 
Critical Test
Twenty-three Indian Ocean nations came 
together on 12 October to test a new warn-
ing communications network that might save 
lives the next time the region is pummeled 
by a tsunami. The $100 million Indian Ocean 
Tsunami Warning and Mitigation System 
performed well, though not awlessly, dur-
ing a simulation modeled on the devastating 
tsunami of 26 December 2004 that killed 
over 230,000 people in 14 countries. Sev-
eral countries also conducted dry runs of 
their own emergency response plans. India, 
Kenya, and Malaysia conducted evacuation 
drills. An actual warning will depend on rap-
idly analyzing data from numerous seismic 
stations, instrumented buoys, and sea-oor 
pressure sensors deployed over the past 
6 years, and spreading the word through 
the networks tested last week. 
The Intergovernmental Oceanographic 
Commission, a part of the United Nations 
Educational, Scientic and Cultural Orga-
nization, which coordinated development 
of the system, declared the test a success. 
Australia, India, and Indonesia will now take 
responsibility for issuing warnings to the 
region. The Japan Meteorological Agency 
and the United States Pacic Tsunami 
Warning Center have issued regional 
warnings since 2005.
Moscow  4
Russian Scientists Rally to Protest 
Funding Freeze
Hundreds of researchers, many in lab 
coats, rallied in Moscows Pushkin Square 
13 October to protest a funding freeze at 
Russias two grant organizations and on 
procurement regulations that they call 
major obstacles to research. The rally was 
organized by the trade union of the Russian 
Academy of Sciences (RAS) and the Young 
Scientists Council, together with associa-
tions of Moscow State University students, 
and young scientists. 
The Russian government recently froze 
the budgets for Russias two funding agen-
cies, the Russian Foundation for Basic 
Research (RFBR) and the Russian Founda-
tion for Humanities (RFH), leaving only 
$200 million for both agencies. Protestors 
urged the government to restore the old 
rule, under which RFBR received 6% of the 
overall budget for civilian science and RFH 
1%. The protestors also demanded radical 
reform of laws governing public procure-
ment, which severely limit grantees freedom 
London  1
Royal Society: Plan Ahead 
For Nuclear Power 
Despite projections of low nuclear power 
growth in Europe and the United States, 
a renaissance of nuclear power construc-
tion in China, Southeast Asia, and Russia 
is likely, Britains Royal Society notes in a 
report released 12 October. As a result, the 
report says, governments and international 
bodies need to develop long-term policies 
to account not only for safety but also for 
security, proliferation risk, and fuel cycle 
management.
Spent fuel can no longer be an after-
thought and governments worldwide need to 
face up to this issue, Roger Cashmore, head 
of the U.K. Atomic Energy Authority and 
chair of the Royal Society working group 
that drafted the report, said in a statement.
The panel recommends that countries 
place their civil nuclear programs under 
international safeguards run by the Inter-
national Atomic Energy Agency (IAEA), so 
that spent fuel cannot be diverted for weap-
ons use. Countries that already have nuclear 
weapons should separate their civil and 
military nuclear programs. It also suggests 
setting up a World Nuclear Forum, made up 
of CEOs and government leaders, to discuss 
nuclear developments and responsibilities.
http://scim.ag/nuclearUK
Sriharikota, India  2
Monsoon Satellite Promises 
Data Deluge
The Indo-French satellite Megha 
Tropiques, tasked with helping scientists 
understand the water and energy balance 
that controls monsoons, launched success-
fully 12 October from the Indian space port 
1
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5
6
2
3
AROUND THE WORLD
Deluged. Damage in Phuket, Thailand, 
following the 2004 tsunami.
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   295
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Making the Invisible Visible 
For her colorful microscopy images that reveal the once-hidden secrets of cells, biochem-
ist Nancy Kedersha has won the Lennart Nilsson Award for scientic and medical photog-
raphy, presented annually in honor of Swedish photographer Lennart Nilsson. The award 
comes with a cash prize of SEK 100,000 (about $15,500). Kedersha will receive the award 
at a ceremony 8 November at the Berwald Hall in Stockholm, Sweden. 
Nancy Kedershas colour images open our eyes to the smallest components of life, 
the award selection panel stated in a press release 14 October. With the aid of a confocal 
microscope, she has turned biological data into an artistic experience.
Kedersha is a researcher at Harvard Medical School and director of the confocal 
microscopy core at Brigham and Womens Hospital in Boston. While working in the lab of 
biochemist and cell biologist Leonard Rome at the University of California, Los Angeles, 
in the 1980s, Kedersha developed a technique to stain and photograph cells to reveal 
their inner workings. Using this technique, she co-discovered a mysterious organelle 
called a vault that exists in everything from humans to slime molds. She has continued 
to develop techniques to identify different cell functions, distinguish healthy cells from 
cancerous ones, and observe cells dividing. 
THEY SAID IT
 If Im going to take money 
from a citizen to put into 
education then Im going 
to take that money to create 
jobs. So I want that money 
to go to degrees where 
people can get jobs in this 
state. Is it a vital interest 
of the state to have more 
anthropologists? I dont 
think so. 
Florida Governor Rick Scott (R) to the 
Sarasota Herald-Tribune on 10 October.
to spend the money as they see t. 
This rally is a warning, says Evgeny 
Onishchenko of the RAS Institute of Phys-
ics, one of the organizers. We want to make 
it clear that if nothing is done to meet our 
demands, there will be much more serious 
rallies of researchers all over the country. 
Klong Luang, Pathum Thani, Thailand  5
Thai Floods Spare Research Park
Flood waters creeping toward Thailands big-
gest research park forced the evacuation of 
dozens of public and private labs last week. 
The Thailand Science Park, 30 kilometers 
north of Bangkok, is home to 2700 employ-
ees working in four national research insti-
tutes under the National Science and Tech-
nology Development Agency as well as in 
the labs of 60 private companies. 
The campus closed 13 October; although 
the science park was still dry on Monday, 
it remained closed through 19 October due 
to high water in surrounding areas. The 
ooding, the worst in 50 years, has already 
claimed more than 300 lives and, according 
to a Businessweek report, caused over 
$5.1 billion in damage. 
Washington, D.C.  6
House Panel Lays Out 
Spending Preferences
A climate-science satellite, some tech-
nology commercialization efforts, and a 
chemical risk assessment program are all 
among the federal R&D programs that 
Republican leaders of the House of Repre-
sentatives Committee on Science, Space, 
and Technology would cut to rein in the 
U.S. budget decit. The ideas, which also 
include protecting the core budgets of the 
National Science Foundation (NSF) and 
the Department of Energys (DOEs) Ofce 
of Science, were highlighted in an unusu-
ally detailed 14-page letter that the law-
makers sent on 14 October to Congresss 
bipartisan Joint Select Committee on De-
cit Reduction, which must devise a plan to 
trim at least $1.2 trillion from the decit 
over 10 years. 
In general, the Republican lawmakers 
took a back-to-basics approach, arguing 
for protecting traditional science pro-
grams while trimming many newer efforts 
championed by the Obama Administra-
tion. They took an especially dim view 
of climate-related research; taxpayers 
could save $149 million over 5 years, 
for instance, by axing NASAs Orbiting 
Carbon Observatory-2, designed to map 
greenhouse gas emissions. They would 
phase out DOEs Advanced Research Proj-
ects AgencyEnergy (ARPA-E), saving 
$180 million. All told, they proposed cuts 
totaling $1.5 billion.
The panels ranking Democrat, mean-
while, penned a less specic plea for spar-
ing the knife and fattening the federal purse. 
When it comes to funding science, it is 
critically important for the committee to 
include serious revenue enhancements in its 
set of recommendations, wrote Representa-
tive Eddie Bernice Johnson (DTX). Neither 
letter is likely to have a major impact on the 
decit committee, which faces a 23 Novem-
ber deadline for delivering its plan.
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org 296
NEWS OF THE WEEK
entry, Microstructure-Property rela-
tionships in Ti2448 components pro-
duced by Selective Laser Melting, 
Miller, 32, ies in silvery spandex 
and a cape as he dances with women 
representing titaniums alpha and 
beta crystalline forms. He receives 
$1000 and a trip to Belgium to be 
crowned the winner on 22 November 
at TEDxBrussels.
Category winners include X-ray 
Crystal Structure of Human Protein 
Phosphatase, by FoSheng Hsu of 
Cornell University (Chemistry); Smell-
Mediated Response to Relatedness of 
Potential Mates, by Cedric Tan of the Uni-
versity of Oxford in the United Kingdom 
(Biology); and A Study of Social Inter-
activity Using Pigeon Courtship, 
by Emma Ware of Queens University 
in Canada (Social Science). Videos of 
this years 55 Ph.D. dances are at 
www.gonzolabs.org/dance.
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CSI: Amphorae?
What did amphorae, the ubiquitous ceramic 
jugs of the ancient Mediterranean maritime 
world, actually contain? To nd out, mari-
time archaeologist Brendan Foley of the 
Woods Hole Oceanographic Institution in 
Massachusetts and colleagues turned to a 
CSI-like method: swiping the insides of the 
amphorae with a swab. They swabbed nine 
5th to 3rd century B.C.E. amphorae for DNA 
and compared it with snippets of DNA from 
various plants.
They identied DNA from a range of 
commodities, including olive oil, olives, 
and wine, as well as traces of DNA from 
oregano, thyme, mint, and juniper, the team 
reports in a study published online this 
month in the Journal of Archaeological 
Science. Eight of the nine amphorae bore 
DNA from a complex mixture of foods, 
suggesting that amphorae were reused, 
Foley says.
Not everyone is convinced that the tech-
nique works, however. It is remarkable 
that an amphora should release endog-
enous DNA by simply swabbing the sur-
face, Oliver Craig of the University of York 
in the United Kingdom said via e-mail. 
Craig, who specializes in recovering DNA 
and other molecules from ancient artifacts, 
says he would need to see more control 
tests to be convinced. 
http://scim.ag/CSIamphora
Nearly Intact Dino Fossil Found in Germany
An exceptionally well-preserved baby dinosaur, with traces of skin and protofeathers, will 
be the main attraction at a fossil and gem show next week in Munich. The juvenile theropod, 
which lived between 145 million and 150 million years ago and was probably less than a year 
old when it died, is 98% intact. That makes it the most nearly complete dinosaur ever found 
in Europe, says Oliver Rauhut, curator at the Bavarian State Collection for Palaeontology and 
Geology in Munich, who led the rst examinations of the fossil. 
The fossils hairlike protofeathers may help researchers understand how and when feath-
ers evolved. The roughly 70-cm specimen, not yet fully classied or named, was unearthed 
near the Bavarian town of Kelheim and has been registered as a German cultural artifact, 
which means that it cant leave the country. The mineral show will display the fossil for 4 
days starting 27 October; a spokesperson for the show has said the unnamed owner plans 
to lend the fossil to a museum.
FINDINGS
Dances With Titanium
Fifty-ve scientists around the world moon-
lighted as choreographers for Sciences 
fourth annual Dance Your Ph.D. contest
and the results are in. This years winning 
dances were based on protein x-ray crystal-
lography, fruit-y sex, and pigeon courtship, 
each scooping $500 prizes. 
The grand winner, announced 20 Octo-
ber, is Joel Miller, a biomedical engineer 
at the University of Western Australia in 
Perth. Millers dance, which won the phys-
ics category, depicts his work with lasers 
to create titanium alloys strong and ex-
ible enough for long-lasting hip replace-
ments. We didnt have a video camera, 
says Miller. So he and his friends converted 
2200 still photographs of the dance into 
stop-motion animation. In his winning 
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   297
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BY THE NUMBERS
1 billion tons  Amount of extra 
food that that could be grown on 
agricultural lands now devoted to 
animal feed and biofuel produc-
tion, according to an analysis in this 
weeks Nature.
200,000 amps  Maximum 
power generated by a new airplane 
industrysponsored lab at Cardiff 
University that studies the effects of 
lightning on materials. An average 
lightning strike generates 10,000 to 
30,000 amps.
Random Sample
The Story Is Dead. Long Live the Story.
Artist  and  self-styled  experimental  philosopher 
Jonathon Keats is hoping to persuade the art world to 
join scientists in the Copernican Revolutionnearly 
5 centuries late. In 1543, Nicolaus Copernicus made the 
humbling observation that the Earth revolves around 
the sun. Modern physicists often cite the Copernican 
principle that, as natures rules are the same every-
where, the human viewpoint isnt unique.
But  the  art  world,  Keats  says,  is  still  stubbornly 
Ptolemaic, in that it emphasizes the exceptionalism 
of humans and centers on stories about ourselves. So, 
in The First Copernican Art Manifesto, an exhibit that 
opened Thursday at the Modernism gallery in San Fran-
cisco, California, Keats will feature art that reects banal, average truths about the universe. 
The pieces dont assume a human audience or viewpointand they dont aim to appeal 
to us, either. One canvas is painted a bland tan, the average color of the starlight of all stars 
measured by astronomers. Hydrogen gas released from glassware suspended above otherwise 
empty pedestals assumes a form invisible to human eyes. A quarter of the notes in a once-
orderly Bach composition are rearrangedreecting the increasing entropy of the universe 
since its tidy, prebig bang singularity.
Although not for humans, the exhibition is aimed at a particular demographic, in a way. 
Were the aliens to land and see our show, they wouldnt say, Now I understand humanity,  
Keats says. Theyd say, Now I have a better understanding of the universe.  The exhibit runs 
through the end of November.
Cute TV Chimps May Harm 
Wild Brethren
Some entertainment industry moguls claim 
that chimpanzees dressed in clothes and 
clowning around fosters sympathy for the 
species. But a study published 12 October 
in PLoS ONE suggests the opposite: Peo-
ple who watch such shows or ads decide 
chimpanzees are abundant in the wild and 
dont need further protection. 
Evolutionary anthropologist Brian Hare 
at Duke University in Durham, North Caro-
lina, and colleagues asked 165 people to 
answer a questionnaire about the status of 
chimpanzees in the wild after watching tele-
vision ads for products such as toothpaste 
and soft drinks. Mixed in with the ads was 
one of three short lms about chimpanzees. 
One showed Jane Goodall urging for their 
protection; another showed footage of chim-
panzees in the wild; and the third showed 
chimpanzees acting in ads.
The results suggested absolutely no 
support for the familiarity hypothesis, 
 
t 
-
Hare says. More than 35% of 
those who watched the humor-
ous ads thought individuals 
should have the right to own a 
chimpanzee as a pet, compared 
with only 10% of those who 
watched the two other lms. 
Those who watched the enter-
tainment chimps were also least 
likely to donate to a conserva-
tion charity.
http://scim.ag/chimpads
Black Death Spawned 
Modern Plague 
These skeletonsexcavated in the 
1980s from a 14th century graveyard in 
Londonbelonged to six of the estimated 
30 million people who died from the Black 
Death, the plague epidemic that swept 
Europe between 1347 and 1351. Research-
ers used teeth from the same graveyard
home to 2500 plague victimsto recon-
struct 99% of the genome of Yersinia 
pestis, the bacterium that causes plague. 
An analysis of that microbial DNA pub-
lished online 12 October in Nature sug-
gests that Y. pestis strains currently circu-
lating around the world are all descendents 
of the medieval strain believed to have 
killed 30% to 60% of Europes population. 
The 14th century genome closely resem-
bled those of modern strains and did not 
have any obvious unique mutations that 
might explain its unprecedented virulence. 
Other factorssuch as the populations 
susceptibility or the ecology of rodents 
and eas, which help spread the disease
were probably responsible for the medi-
eval calamity, the team concludes.
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  298
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Sometimes  just  meeting  expectations  is  a 
major achievement. Initial, eagerly awaited 
results  from  the  worlds  first  large-scale 
trial of a malaria vaccine, carried out at 11 
sites in seven African countries, show that 
it reduced episodes of the disease by about 
half in babies and toddlers. That conrms 
the  efcacy  seen  in  earlier,  much  smaller 
trials of the experimental vaccine, so far the 
only one to show signicant benet against 
malaria in real-world settings.
The new ndings keep the candidate on 
track to become the rst licensed vaccine 
against the disease, says Christopher Plowe, 
a malaria vaccine expert at the University of 
Maryland School of Medicine in Baltimore, 
who is not involved in the trial. Even a par-
tially effective vaccine, used in combination 
with other tools like bed nets, could curtail 
malarias  massive  death  toll  signicantly, 
experts say. But the vaccine will be expen-
sive by developing-world standards, and its 
cost-effectiveness is yet to be determined. 
I  am  thrilled,  says  Joe  Cohen,  one 
of  the  vaccines  original  developers  and 
leader  of  the  malaria  vaccine  project  at 
GlaxoSmithKline  (GSK)  Biologicals  in 
Rixensart, Belgium. The fact that the huge 
trial  confirms  results  from  smaller  pre-
decessors  is  fabulous,  he  says.  Robert 
Newman, head of the World Health Orga-
nizations  (WHOs)  malaria  program, 
agrees. The results are in line with what 
we expected. But one fears they wont hold 
up, so in line is very encouraging.
The rst round of results was published 
online  on  18  October  by  The  New  Eng-
land  Journal  of  Medicine;  they  were  also 
announced by Bill Gateswho called them 
phenomenalat a Seattle meeting hosted 
by  the  Bill  &  Melinda  Gates  Foundation, 
which has given more than $200 million to 
support trials of the vaccine. The data show 
that in 6000 children aged 5 to 17 months, 
three doses of the vaccine cut the risk of any 
episode of malaria by 56% and the risk of 
severe disease by 47%. Thats far from the 
90% efcacy that most vaccines against viral 
and bacterial disease achieve. But the Plas-
modium falciparum parasite, with its multi-
ple life stages, is a much more difcult target, 
and no one expected a rst-generation vac-
cine to be more than partially effective. This 
vaccine  will  not  be  a  magic  bullet  against 
what is a very, very difcult disease, Cohen 
says. It is one weapon to be added to an arse-
nal of other interventions.
The vaccine, called RTS,S, was developed 
in 1987 by researchers working for a prede-
cessor  to  GSK  Biologicals.  It  contains  an 
engineered protein that combines a protein 
fragment from P. falciparum and a protein 
from  the  hepatitis  B  virus  that  helps  trig-
ger a strong immune response. The vaccine 
is designed to block the parasites ability to 
infect the liver and mature there.
After early human trials in 1997 showed 
promising  resultsprotecting  six  of  seven 
adult  volunteersGSK  entered  a  public-
private partnership with the PATH Malaria 
Vaccine Initiative (MVI) to further develop the 
vaccine. The rst eld trials in 2000 children 
in Mozambique, launched in 2003, showed 
that  the  vaccine  lowered  the  risk  of  devel-
oping  malaria  symptoms  by  30%,  with  no 
severe side effects (Science, 22 October 2004, 
p. 587). Since then, phase II trials in Mozam-
bique, Kenya, and Tanzania have consistently 
shown that the vaccine can cut the number of 
malaria episodes by between 35% and 53% 
(Science, 12 December 2008, p. 1622).
The  phase  III  trialthe  final  test
enrolled  more  than  15,000  babies  aged 
6 to 12 weeks and toddlers between 5 and 
17 months across sub-Saharan Africa. All 
were scheduled to receive three doses, each 
1  month  apart;  a  subgroup  will  receive  a 
booster  dose  18  months  later. The  results 
announced  this  week  are  for  the  toddlers 
and  cover  the  12  months  after  their  first 
shot. (Infants were enrolled slightly later, so 
results from that group wont be available 
until the end of 2012.) Children who missed 
one or two of the doses were almost as well 
protected  as  those  who  received  all  three 
shots, the researchers report.
The vaccine also looks fairly safe. Chil-
dren who received the vaccine had a slightly 
higher  rate  of  seizures  than  those  who 
received the control injection, a rabies vac-
cine. But the independent safety board that 
keeps  watch  over  the  trial  has  not  raised 
any concerns, says MVI Director Christian 
Loucq. Children enrolled in the trial had a 
very low risk of dying from malariaeven 
if  they  received  the  control  injections
mainly because clinics put in place proce-
dures  to  detect  and  treat  cases  as  soon  as 
possible. There were only 10 malaria deaths 
in the rst 2 years of the study, Cohen says.
In  a  separate  analysis,  the  researchers 
looked at the rate of severe malaria to date 
in all 15,460 children enrolled in the study; 
they found that the vaccine reduced the rate of 
severe, life-threatening disease by 35%. That 
hints that effectiveness might be lower in the 
babies, but Loucq and Cohen caution that the 
number is very preliminary.
The  babies  received  their  doses  at  the 
same time they receive the standard infant 
vaccinations recommended by WHO. Add-
ing the malaria vaccine to existing vaccina-
Vaccine Trial Meets Modest 
Expectations, Buoys Hopes
MALARI A
Promising jab. A baby receives a dose of the experi-
mental malaria vaccine at a trial site in Kili, Kenya.
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  299
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tion schedules would be the most practical 
approach if the vaccine is to be widely used, 
and smaller-scale trials have suggested that it 
is effective and safe when given along with 
the other shots.
The trial will continue until 2014 and will 
follow the children until 30 months after their 
third dose. Once the full results are unblinded, 
researchers will know more about how long 
protection lasts and will also be able to com-
pare the vaccines performance at different 
study  sites,  which  have  different  rates  and 
seasonal  patterns  of  malaria  trans mission. 
That  could  help  governments  and  public 
health  experts  decide  where  RTS,S  might 
have the most impact. The complex vaccine 
is expensive to make, and its cost-effective-
ness is a major issue, says Scott Filler of the 
Global Fund to Fight AIDS, Tuberculosis and 
Malaria.  The  key  question  is  going  to  be 
cost, he says, given the limited funds avail-
able for ghting malaria.
GSK,  which  has  invested  more  than 
$300 million in RTS,S to date, has pledged 
to  keep  the  price  as  low  as  possiblejust 
manufacturing costs plus a small return to 
be  reinvested  in  development  of  second-
generation  malaria  vaccines  or  vaccines 
against  other  neglected  tropical  diseases. 
Even so, a full vaccine course is likely to cost 
more than other prevention methods, such as 
insecticide-treated  bed  nets,  which  also 
offer  partial  protection.  Many  countries 
have already rolled out massive net distribu-
tion projects, and 75% of the children in the 
trial slept under a net, Cohen says; the results 
show that the vaccine can provide an extra 
layer of protection on top of the nets, he says. 
WHO is expected to take all such issues 
into  account  when  it  drafts  policy  recom-
mendations for use of the vaccine after the 
trials nal results come in. The vaccine has 
incredible  potential  to  reduce  suffering, 
Filler says, but deciding how and where to 
use it will take much more work. These are 
going to be incredibly challenging questions 
for which wethe community as a whole
dont have answers yet.
GRETCHEN VOGEL AND LESLIE ROBERTS
A  $70-million-a-year  program  launched 
7  years  ago  at  the  National  Institutes  of 
Health  (NIH)  to  help  academic  research-
ers move into industry-style drug discovery 
may soon be forced to scale back sharply. 
NIH  Director  Francis  Collins  has  been 
one of its biggest champions. But the NIH 
Molecular  Libraries,  according  to  plan, 
must be weaned starting next year from the 
NIH  directors  office  Common  Fund  and 
nd support at other NIH institutes. In a time 
of tight budgets, nobody wants it.
The fate of the Molecular Libraries pro-
gram became an extremely sensitive politi-
cal issue earlier this year when NIH realized 
it would not be easy to nd a new home for 
the program, said one NIH ofcial speaking 
on background. It illustrates the complexity 
of moving projects out of the Common Fund, 
says  the  funds  overseer,  James Anderson, 
director of NIHs Division of Program Coor-
dination, Planning, and Strategic Initiatives. 
Obviously the process would be easier if 
NIHs budget were growing, he says.  
The Molecular Libraries began as a large 
piece of the NIH Roadmap, a set of cross-
cutting  initiatives  announced  in  2003  by 
thenNIH  Director  Elias  Zerhouni.  (The 
Roadmap later became the Common Fund.) 
As  described  by  Collins,  who  was  then 
the  genome  institute  director,  academic 
researchers  would  submit  protein  or  cell 
assays to a set of academic screening cen-
ters, which would be paid by NIH to look 
for biological interactions with thousands 
of chemicals. Chemists would then rene 
these hits into research probes, some 
of which could become drug candidates. 
Although some industry scientists were 
skeptical of government-led drug research, 
NIH  scaled  up  the  program  from  a  pilot 
phase  in  2008  (Science,  8 August  2008, 
p.  764).  The  program  now  includes  four 
large  screening  centersone  part  of 
NIHs  in-house  research  program,  the  rest 
extramuraland  five  supporting  centers. 
They have produced more than 240 probes, 
one of which is now in clinical trials as a mul-
tiple sclerosis (MS) drug. Hugh Rosen, direc-
tor of a center at Scripps Research Institute in 
San Diego, California, said papers in top jour-
nalsincluding those on the MS drugshow 
that the program has transformed academic 
chemical discovery and target validation.
The centers were told, however, that their 
Common Fund money would end in 2014 and 
that they would have to nd other sponsors. 
Only the intramural center has found a poten-
tial home so far: It will move to NIHs planned 
National Center for Advancing Translational 
Sciences, if Congress approves. 
The extramural centers arent so lucky. 
Their Common Fund 
awards  will  drop  by 
33%  next  June  and 
another  33%  in  June 
2013. Other institutes 
are reluctant to pick 
them up because they 
need the money for research grants, accord-
ing to Molecular Libraries program director 
Carson Loomis. Loomis says NIH intends to 
replace some of the declining money with 
new grants to users of the extramural cen-
ters focused on drug discovery. Still, he says, 
there will be some belt-tightening. 
John Reed, head of the Sanford-Burnham 
Medical Research Institute screening center 
in San Diego, which receives about $16 mil-
lion a year from the Common Fund, says his 
center has so far attracted only modest fund-
ing from drug companies. He expressed frus-
tration with the Common Fund process. NIH 
has put a huge investment into [the Molecular 
Libraries], and its running very well, he says. 
If  theres  not  a  long-term  commitment  to 
keep it available to the academic community, 
why did we make this hundreds of millions of 
dollars investment?              JOCELYN KAISER 
Drug-Screening Program Looking for a Home
NATI ONAL  I NSTI TUTES  OF  HEALTH
2
a
th
Screen test. NIHs 
Molecular Libraries has 
yielded scores of probes.
Long-term investment. Joe Cohen of GSK Biologicals 
has been working on the RTS,S vaccine for 24 years.
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  300
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The U.S. Ofce of Naval Research (ONR) has 
joined forces with the Texas-based National 
Math  and  Science  Initiative  (NMSI)  to 
increase the number of high school students 
taking rigorous science and math courses. Its 
$1.1  million  grant,  announced  last  month, 
could prompt a closer look at one controver-
sial aspect of the initiatives approach: paying 
students to do well on standardized tests.
Launched  in  2007  with  funding  from 
major corporations and foundations, NMSI 
gives money to school districts that agree to 
follow its tightly scripted program. The goal 
is to boost participation in Advanced Place-
ment (AP) classes, a curriculum designed 
by the nonprot College Board to be on par 
with  entry-level  college  courses. 
The  NMSI  program,  which  targets 
low-achieving and low-income high 
schools  with  large  minority  popu-
lations, assumes that these students 
can handle more challenging mate-
rial if given the chance. NMSI of-
cials say that is already happening: 
In the midst of a nationwide surge 
in  AP  test-taking,  the  number  of 
minority and female students pass-
ing AP tests at 228 NMSI-sponsored 
schools this year increased four to 10 
times faster than for the country as a 
whole (see graphic).
Most  of  NMSIs  approach  rep-
resents  education  orthodoxy:  extra 
class  time  for  students,  additional 
resources,  and  special  training 
for  teachers.  But  there  is  less  evi-
dence behind another core element, 
namely,  cash  incentives.  Students 
receive from $100 to $500 for pass-
ing an end-of-the-year test, and their 
teachers also get bonuses for each stu-
dent who succeeds and for teaching 
AP classes. NMSI pays for success in only 
English,  math,  and  science  courses  (tests 
are  offered  in  34  subjects).  But  students 
may take half a dozen or more AP courses 
in  those  subjects  during  their  high  school 
careers, so the money can add up.
ONRs investment puts the Navy ahead 
of  the  curve  on  national  education  policy. 
The  Obama  Administration  has  no  offi-
cial position on the use of cash incentives, 
and Congress has never addressed the topic 
in legislation. At the same time, Education 
Secretary Arne Duncan has voiced support 
for the concept as a tool for raising student 
achievement, and a small departmental pro-
gram to increase participation in AP courses 
allows ofcials to give money directly to stu-
dents. However, only two of the 55 current 
grantees are doing so. 
The Navys STEM (science, technology, 
engineering,  and  mathematics)  education 
budget is expected to double in 5 years, to 
more than $100 million, reecting its con-
cern about lling science- and technology-
based Navy jobs. Michael Kassner, head of 
the Navys STEM ofce, says NMSI could 
become  a  big  part  of  that  investment  if 
the 3-year pilot, which supports three pub-
lic schools in Virginia and Hawaii that enroll 
large  numbers  of  students  from  military 
families,  is  able  to  help  prime  the  pump. 
We know that students whose parents are 
in the military are more likely to go into the 
military, he adds. 
Kirabo  Jackson,  a  labor  economist  at 
Northwestern  University  in  Evanston,  Illi-
nois, has looked at the Texas program that 
spawned NMSI. His 2008 study, perhaps the 
only one to examine the role of incentives in 
the population that NMSI is targeting, found 
that the strategy increased AP participation 
rates and boosted the number of students with 
high scores on national college entrance tests. 
At the same time, the program didnt increase 
high school graduation rates or the number 
of students taking college entrance exams. 
That nding suggests its more likely to help 
high achievers already headed to college than 
to raise the aspirations of those who hadnt 
planned to continue their education.
Still,  his  overall  assessment  is  posi-
tive: Its one of the few programs that does 
something good for these students, Jackson 
says. Most programs havent been evalu-
ated rigorously. And I dont know if it can be 
expanded to other settings, with other popu-
lations. But if a school district had $1 mil-
lion to spend, I think a program like this is a 
good investment.
A 2010 study by economist Roland Fryer 
Jr.  of  Harvard  University  delivers  a  much 
more sobering message about the value of 
cash incentives for younger students. Fryer 
conducted a randomized trial of experimen-
tal programs in four large urban school dis-
tricts involving 38,000 children from grades 
two through nine. Although the program ele-
ments varied greatly from one district to the 
next, he found that paying for outputs, such 
as test results, didnt work and in some cases 
resulted in lower scores. On the other hand, 
paying students for inputsshowing up for 
class, staying on task, reading a certain num-
ber of bookshad a positive effect, he writes 
in a paper posted by the National Bureau of 
Economic Research.
Teacher unions have generally been very 
leery of incentives or bonuses. In addition to 
clashing with most labor agreements, they 
are  regarded  as  undermining  the  learning 
process. And almost none of these incentive 
programs have worked, says a spokesperson 
for the United Federation of Teachers, which 
represents New York City schools. 
A  program  serving  31  New York  City 
schools  that  is  otherwise  modeled  after 
the  Texas  and  NMSI  efforts  omitted  the 
teacher incentives after the union declined 
to participate. And this month ofcials for 
the  program,  called  REACH  (Rewarding 
Achievement), dropped the student incen-
tives in response to a nancial squeeze. We 
found that it prompted more students to take 
AP courses, but we didnt see the magnitude 
effect  that  we  had  hoped,  says  Kathrine 
Mott, REACHs executive director. REACH 
will  continue  to  offer  professional  devel-
opment for teachers, Saturday classes, and 
classroom grants, she adds.
JEFFREY MERVIS
Navy Dives Into Program Offering Cash for Good Scores
U. S.   SCI ENCE  EDUCATI ON
Students taking AP tests
P
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g
e
 
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e
a
s
e
 
o
f
 
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a
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s
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s
c
o
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e
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FEMALES*
AFRICAN-
AMERICAN
AND 
HISPANIC**
OVERALL**
0
50
100
150
200
250
23%
124%
50%
216%
20%
144%
  *Math, Science
**Math, Science,
   and English
U.S.
Total
NMSI
Schools
Advancing AP. NMSI ofcials say that test results demon-
strate the value of cash incentives in boosting the number of 
high school students taking and passing AP courses.
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In  Chinas  booming  economy,  there  are 
many ways to get rich. For a husband-and-
wife team on Hainan, an island off Chinas 
southern  coast,  scientific  publishing  was 
their cash cow. For 7 years, Guo Hong and 
Fu Li operated 20-some journals, collecting 
a reported $1.5 million in publication fees 
from thousands of contributors. They solic-
ited  papers  through  elaborate  Web  sites, 
offering a discount on the publication fees 
common  in  China.  But  the  journals  were 
fake,  provincial  authorities  allege.  Upon 
receiving  submissions,  the  couple  would 
print up only a few copiesjournal titles 
included  Chinese  Applied  Nursing  and 
Chinese  Medicine  Forumto  send  to  the 
author. Guo and Fu were detained in March; 
prosecutors have not yet led charges. 
The  highly  publicized  takedown  is  one 
of several recent efforts to clean up Chinas 
academic publishing industry. In a country 
where low publication standards abound and 
every university or institute, it seems, has its 
own journal, the Chinese government is get-
ting serious about raising standards. Although 
the Hainan journals fraud is an outlier, its 
symptomatic of a larger problem: slapdash 
and irrelevant publications read by next to no 
one. At most Chinese journals, the academic 
level is not high, Li Dongdong, vice director 
of the General Administration of Press and 
Publication (GAPP), which regulates publi-
cations in China, noted in a speech in Decem-
ber. She estimated that two-thirds of journals 
are not market-oriented.
As Chinese science barrels ahead, a few 
of its journals are getting international atten-
tion, and leading Western publishers have set 
up shop on the mainland in response. But the 
countrys 4700 scientic periodicals include a 
hefty number of what the Chinese press refers 
to as trash journals. Despite being second 
only to the United States in total papers pub-
lished from 2006 to 2010, China ranked at the 
bottom of the top 20 countries for citations 
per article over the same period, with just 1.47 
citations on average, according to Elseviers 
SciVerse Scopus database and SciVal Spot-
light country matrix, compared with 5.16 for 
the United States. It doesnt help that many 
institutions in China offer fat rewards for pub-
lishing in overseas journals with high impact 
factors. For example, according to its Web 
site,  Guangzhou  Medical  University  doles 
out 300,000 yuan ($47,000) to lead authors 
on papers in journals with impact factors of 
at least 15a level no Chinese journal has 
attained.  (In  Thomson  Reuterss  Journal 
Citation Reports, top-ranked journals in cat-
egories such as cell biology and biochemistry 
can show impact factors of over 30.)
As an antidote, GAPP has begun rolling 
out a series of reforms aimed at boosting the 
prestige of Chinese publishing. GAPP has 
been given heaps of money to spend, says 
Torsten Weise, a Berlin-based consultant who 
advises  foreign  publishers  on  operating  in 
China. In the past 2 years, GAPP has secured 
billions of dollars in loans from state banks, 
with the major goal, Weise says, of inter-
nationalization: building journals and pub-
lishers capable of becoming multinational.
Chinas 12th 5-year plan, in effect since 
March, sets a heady goal for journals. It calls 
for making cultural productionincluding 
media and publishinga pillar industry. 
GAPP has moved swiftly. Earlier this year, 
the agency closed six obscure publications 
and  reprimanded  two  others  for  violations 
that included indiscriminate printing of up 
to 200 papers per issue, over the limits set by 
publishing licenses. Then last summer, of-
cials unveiled China Science and Technology 
Media Group, one of a handful of agship 
publishers due to be rolled out over the next 
few years to compete with foreign rivals such 
as Wiley, Elsevier, and Springer. Li has talked 
about  GAPP  supporting  a  group  of  select 
academic journals; editors are unclear when 
funding might materialize.
The malaise has deep roots. The prolifera-
tion of journals is tied to the danwei, or work 
unit, system put in place after 1949. As the 
government brought institutions under cen-
tral control, academic work unitsoften uni-
versity departments or instituteslaunched 
journals to publish their scholars work.
Fast-forward  to  the  1990s.  With  Chi-
nese science opening up, academic centers 
shifted course and began rewarding scientists 
for  publishing  in  journals  listed  in  indices 
that track citation rates. Pressure to publish 
piled up, and although only a few thousand 
Chinese papers a year then made it into jour-
nals indexed by Thomson Reuters, authors 
seeking to get into print in both Chinese and 
English-language outlets proliferated. Medi-
ocre danwei-linked journals gladly solicited 
papers  from  outside  scientists  and  began 
charging steep publication fees. (These can 
now top $1000.) And so the early journals 
persisted,  constituting  what  Cong  Cao,  a 
scholar of Chinese science at the University 
of Nottingham, U.K., calls a phenomenon 
with Chinese characteristics.
Today,  the  few  stars  that  have  emerged 
are published in English and focus on areas 
in which China is strong, such as cell biol-
ogy,  nanoscience,  and  materials  science. 
They have risen quickly: In 1999, the high-
est impact factor of any Chinese journal was 
0.5 (Science, 26 November 1999, p. 1683). 
Today,  Chinas  top  indexed  journal,  Cell 
Research, has an impact factor of 9.4.
Chinas leading journals have made their 
mark by bringing on international editorial 
boards, wooing editors from top-shelf West-
ern  publicationsCell  Research  poached 
deputy  editor  in  chief  Li  Dangsheng  from 
Cell in 2006and taking stabs at branding, 
such  as  shedding  China-specific  names  in 
favor of more international monikers. Oth-
ers, including Chinese Medical Journal and 
Science China Life Sciences, are experiment-
ing with open-access platforms. We have to 
change the way journals are run, says Gang 
Pei, editor-in-chief of Cell Research. He has 
cultivated  relationships  with  societies  and 
accelerated  response  time  for  submissions 
from leading researchers.
The vast majority of journals have little 
hope of following that recipe. Their day of 
reckoning is not long off. There is no need 
to keep poor-quality journals around, says 
Meng  Zhao,  development  editor  at  Neural 
Regeneration Research. By administrative 
measures or by market measures, Pei says, 
there will be some kind of cleanup. 
MARA HVISTENDAHL
China Looks to Purge Academia 
Of Trash Journals
SCI ENTI FI C  PUBLI SHI NG
Raising the bar. Gang Peis Cell Research is Chinas 
top indexed journal.
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  302
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The experienced hunter hurled or thrust his 
spear at the left side of the 3-ton adult male 
mastodon. The bone point passed through 
25  to  30  centimeters  of  hide  and  muscle, 
then pierced a rib bone. That wound alone 
likely did not kill the massive animal, but 
under the onslaught of a group of hunters, 
the mastodon eventually fell on its left side. 
The victorious hunters then retrieved most 
of their weapons and butchered the animals 
right side. But the valuable spear point 
remained inaccessible, buried under 
the giant carcass. 
That ancient hunters loss is a 
gain for researchers on a different 
kind of hunt: the search for clues 
to the peopling of the Americas. 
Back in the 1970s, archaeologists 
found  the  mastodons  remains, 
complete with rib bone and embed-
ded point, at the Manis Mastodon site 
on  Washingtons  Olympic  Peninsula, 
near  the  Juan  de  Fuca  Strait.  Now  on 
page 351 of this issue, researchers led 
by Michael Waters of Texas A&M Uni-
versity  in  College  Station  use  DNA 
and radiocarbon dating to demonstrate 
that  the  point  came  from  a  mastodon 
bone shaped into a weapon by humans 
and  used  a  startling  13,800  years  ago. 
Thats  nearly  1000  years  before  the 
Clovis culture, known for its distinctive 
stone spear points and long considered 
to be the rst culture in the New World. 
The nd adds to the wave of recent com-
pelling evidence demonstrating an earlier, 
pre-Clovis settling of the Americas (Science, 
25 March, p. 1512). Although a few Clovis-
rst holdouts remain unconvinced, the early 
bone point also suggests that the extinction 
of large mammals such as mastodons and 
mammoths may have begun long before the 
Clovis  people  came  on  the  scene.  This  is 
signicant  because  we  have  so  few  widely 
accepted pre-Clovis sites, says anthropolo-
gist  Daniel  Sandweiss  of  the  University  of 
Maine,  Orono. The  solid  dating  combined 
with the strong evidence for pre-Clovis hunt-
ing on a site near the coast make the results 
particularly important, he adds. 
Waterss team subjected the rib and bone 
barb to a battery of tests, from DNA sequenc-
ing and protein analyses to radiocarbon dating 
and a CT scan. They determined that the barb 
comes from another mastodon and appears to 
resemble the sharpened bone points used to 
kill mammoths, mastodons, and other large 
animals  in  Beringia,  the  land  now  partly 
submerged in the region around the Bering 
Strait. The  first Americans  likely  migrated 
from Beringia as the last ice age gave way to 
warmer temperatures and glaciers retreated. 
For many archaeologists, the debate over 
whether  pre-Clovis  peoples  roamed  the 
Americas is over. Manis is another pre- or 
non-Clovis site on the map, says anthropol-
ogist Tom Dillehay of Vanderbilt University 
in Nashville, who announced his 
own pre-Clovis site in Chile 
back in 1997.
Megafauna like the mast-
odon and its relative the mam-
moth disappeared quickly after 
the  arrival  of  Clovis  points 
13,000  years  ago,  prompting 
some  scientists  to  speak  of  a 
blitzkrieg: a rapid hunting of these giant 
animals  to  extinction.  But  combined  with 
evidence of pre-Clovis mammoth hunting 
at two other North American sites, Waters 
argues that human hunters were already at 
work on killing megafauna before the debut 
of Clovis-style weapons. Other researchers 
agree: The notion of the blitzkrieg move-
ment died with the Clovis-rst paradigm, 
Dillehay asserts. 
Although a well-dated point embedded in 
a mastodon rib seems like a smoking gun
or spearfor the pre-Clovis case, a handful 
of Clovis-rst advocates remain skeptical. 
They say that so far all the evidence, includ-
ing that from Manis, has problems. There 
may  have  been  a  period  of  pre-Clovis 
human  presence  in  North America,  but  I 
wish  I  could  see  a  solid  demonstration  of 
that presence somewhere that doesnt have 
nagging problems, says archaeologist Gary 
Haynes of the University of Nevada, Reno. 
He  questions  whether  the  bone  point  was 
really a human-shaped weapon, saying that 
it  might  have  been  a  piece  of  bone  acci-
dentally driven into the rib. Archaeologist 
Stuart Fiedel of the Louis Berger Group Inc. 
in  Richmond, Virginia,  praises  the  teams 
sophisticated techniques but questions the 
dating. He notes that the mastodons envi-
ronment  had  sources  of  old  carbon, 
including the ocean and geothermal pools, 
that could give a falsely ancient date 
if  the  mastodon  ingested  food  or 
water  from  those  sources.  Waters 
calls this a red herring, however, 
because  the  surrounding  sediment 
age closely matches the bone dating. 
Haynes adds that the oldest Clovis 
sites are only 8 centuries younger 
than Manis. Thus the rib may actu-
ally indicate the earliest beginning 
of the Clovis era, or an immediately 
proto-Clovis stage of human disper-
sal, he says. Proto-Clovis peoples 
in small numbers may have ltered 
south  from  Beringia  as  early  as 
14,000 years ago, he says, although 
their  impact  was  negligible  until 
the arrival of Clovis technology. To 
Waters, such talk of proto-Clovis 
amounts to grasping at straws.
Sandweiss says the implications 
of  the  paper  in  fact  go  beyond  the 
Clovispre-Clovis wrangling. Many 
scientists argue that pre-Clovis peo-
ple  moved  south  along  the  Pacific 
Coast, possibly by boat (Science, 4 March, 
p. 1122). In his view, the location of Manis 
near the ocean is an intriguing hint favor-
ing this idea. The Manis site supports early 
occupation  of  the  coastal  zone,  he  says. 
Waters, who has reported pre-Clovis inte-
rior sites as well, is cautious. We cant say 
these  were  coastal  folks,  he  says  of  the 
Manis  hunters.  But  the  papers  findings, 
Sandweiss  says,  point  to  a  more  wide-
spread and complex early settlement system 
than some might have suspected.
ANDREW LAWLER
Pre-Clovis Mastodon Hunters Make a Point
ARCHAEOLOGY
Big  game.  Archaeologists  say  that  pre-Clovis  hunters  in 
Washington  state  used  a  bone  spear  point  (seen  above 
embedded in a rib) to pierce a mastodon.
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  303
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TASTUBEK, KAZAKHSTANAt a shing camp 
near this village on the Northern Aral Sea, 
a  dozen  small  boats  recently  returned  to 
shore bathed in a soft morning light. Their 
nets bulged with carp, pike, ounder, perch, 
and  a  half-dozen  other  species,  all  edible 
and ready for sale. It was a scene unimagi-
nable just 6 years ago, when the Aralonce 
the worlds fourth-largest lakehad shrunk 
to one-tenth of its original size. Soviet-era 
planners had diverted most of the water that 
owed into the lake from two rivers to irri-
gate cotton, creating three smaller lakes that 
became too salty for most sh. Catches that 
once totaled more than 50,000 tons a year 
plummeted to just 52 tons in 2004.
Now,  since  the  2005  construction  of  a 
$65 million dike, the northern part of the 
Aral  has  become  a  remarkably  healthy 
shery. The  biomass,  or  weight  of  all  the 
sh in the Northern Aral, has soared from 
an estimated 3500 tons in 2005 to 18,000 
tons  today,  says  Zaualkhan Yermakhanov, 
the Kazakh governments regional sheries 
director. And its still growing.
Its been an amazingly fast recovery, 
says  Philip  Micklin,  a  retired  geographer 
from Western Michigan University who has 
been studying the Aral Sea since the 1970s. 
During an expedition last month around the 
Rhode  Islandsized  lake,  Micklin  found 
that salinity levels have dropped and oxy-
gen levels increased since the Kazakh gov-
ernment,  backed  by  the  World  Bank  and 
other donors, built the 13-kilometer earthen 
dike along the Northern Arals southeastern 
edge. The dike traps water from one feeder 
river,  the  Syr  Darya,  and  has  raised  the 
lakes water level by 2 meters and expanded 
its surface area by some 900 square kilo-
meters  (Science,  14 April  2006,  p.  183). 
During his expedition, Micklin found that 
the fresh water had reduced salinity from 
12.3  grams  of  salt  per  liter  in  2005  to 
8 grams and increased water clarity. As a 
result,  not  only  are  fish  becoming  more 
abundant, but aquatic plants and reeds are 
spreading fast.
Prior to construction of the dike, only a 
hardy ounder introduced from the Black 
Sea was able to survive in the northern part 
of the lake. Now, about two dozen species of 
native freshwater sh that high salinity had 
driven into the Syr Daryas delta and adja-
cent lakes have returned to deeper waters 
and are reproducing at a rapid clip. And the 
rebound has been even bigger than World 
Bank planners expected: In the early 2000s, 
says  the  banks  Masood Ahmad,  a  feasi-
bility  study  had  concluded  that  a  revived 
Northern Aral  would  ultimately  produce 
about 2000 tons of sh a yearbut shing 
eets are already catching nearly twice that 
amount. To make sure the stocks continue 
to ourish, Yermakhanov says he is commit-
ted to limiting yearly catches to about one-
third of the total biomassmuch less than 
what is allowed in many managed sheries. 
I know we could sh more, he says, but I 
want to make sure we can grow the biomass 
to at least 40,000 tons.
Kazakhstan,  flush  with  income  from 
oil  and  minerals,  is  now  considering  tak-
ing  the  rescue  effort  a  step  further.  One 
project, backed by Yermakhanov and local 
fishers,  would  raise  the  dike  enough  to 
increase water levels by more than 6 meters, 
expanding the lake surface by about 50%, to 
5000 square kilometers. That plan would 
be  the  best  for  the  ecosystem,  Micklin 
says, but it isnt as politically or economi-
cally attractive as an alternative. That would 
involve digging a canal to bring water back 
to the historic port of Aralsk, which was left 
high and dry by the desiccation. The canal 
plan would benet more people, Micklin 
says. For the moment, however, there isnt 
enough water ow for both. The govern-
ment  announced  last  month  that  it  would 
appoint an expert panel to decide between 
the two options. 
CHRISTOPHER PALA
Christopher Pala is a writer based in Almaty, Kazakhstan.
In Northern Aral Sea, Rebound 
Comes With a Big Catch
ECOLOGI CAL  RESTORATI ON
Aral redux. More freshwater in the Northern Aral 
(above, at top) has enabled shers to once again 
pick a rich catch out of their gill nets (left).
2004
Tastubek
North Aral Sea
2011
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  304
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BLACKSBURG,  VIRGINIAUnlike old sol-
diers, some scientic concepts seem never to 
fade away. Take the hypothetical subatomic 
particle called the sterile neutrino, which 
would be about the oddest bit of matter imag-
inable. For 15 years, researchers have accu-
mulated hints from particle physics, nuclear 
physics, astrophysics, and cosmology that the 
particlea more-elusive cousin of the nearly 
undetectable neutrinosmight be out there. 
But most physicists have found the evidence 
unconvincing, as most of the results pointing 
toward sterile neutrinos are of marginal statis-
tical signicance.
Recently, however, the case for sterile neu-
trinos has grown stronger, bolstered by a new 
analysis of data from nuclear reactors. So last 
month 60 physicists from around the world 
gathered here
*
 to hash out the arguments for 
and against the existence of sterile neutrinos 
and to try to decide whether its worth stag-
ing a dedicated experiment to settle the matter.
Performing such an experiment wont be 
easy. The  hypothetical  neutrinos  are  called 
sterile because they do not interact at all with 
known particles. Youre trying to 
prove  the  existence  of  something 
with no interactions, says Patrick 
Huber,  a  theorist  here  at Virginia 
Polytechnic Institute and State Uni-
versity (Virginia Tech). Its like try-
ing to prove the existence of God. 
Still, he says, its time to gure out 
what it will take to discover or rule out sterile 
neutrinos once and for all. Im afraid well 
have the same workshop 15 years from now 
and will just have more [inconclusive] results 
that dont make the situation any clearer.
Some researchers say the case for a sterile 
neutrino is still half-baked. Im quite skepti-
cal, says Yves Dclais, a neutrino physicist 
at the University of Lyon in France. Each 
piece  of  evidence  itself  is  not  completely 
self-consistent, he says. So Im really con-
cerned  that  there  should  be  more  work  to 
understand  each  anomaly  itself  instead  of 
trying to put together a dedicated experiment 
to look for sterile neutrinos.
Abundant in theory
Ordinary neutrinos are already weird. Nearly 
massless  and  hardly  interacting  with  other 
matter, they are born in weak nuclear decays 
and  interactions.  For  example,  a  neutron 
decays into a proton by emitting an electron 
and an antineutrino. A neutrino can emerge 
when  a  nucleus  of  the  isotope  beryllium-7 
turns into lithium-7 by capturing an electron 
and releasing a neutrino. Trillions of neutrinos 
stream through each of us every second.
Weirder  still,  neutrinos  come  in  three 
avorselectron neutrinos, muon neutri-
nos, and tau neutrinosthat can morph into 
one another. For example, when cosmic rays 
strike the atmosphere, they create particles 
called muons that decay much as neutrons do, 
to produce muon neutrinos. The muon neutri-
nos can then oscillate or mix into other 
avors before reaching Earth, as observed in 
1998 by physicists using a giant subterranean 
detector called Super-Kamiokande in Japan. 
Electron neutrinos from the sun also change 
avor, as physicists at the Sudbury Neutrino 
Observatory in Canada showed in 2001.
A sterile neutrino would be even more elu-
sive than an ordinary neutrino. It would not 
participate in weak interactions and would 
arise only from ordinary neutrinos oscillating 
into a sterile form. As sterile neutrinos would 
not  interact  themselves,  physicists  could 
detect  them  only  indirectly,  by  observing 
ordinary neutrinos disappearing or appearing 
where they are not expected.
Theorists  have  been  think-
ing about sterile neutrinos since 
the late 1960s, when they rst 
suspected  that  neutrinos  from 
the sun oscillated. The morph-
ing meant that neutrinos were 
not massless, and sterile neutri-
nos would help explain how the 
wispy particles put on weight.
Flavor-changing  oscillations  prove  that 
neutrinos have mass because a massless par-
ticle must travel at light speed, and, accord-
ing to Einsteins theory of relativity, at light 
speed  time  stands  still,  making  change 
impossible. The standard model of particle 
Mystery machine. The guts of the LSND detector, 
which may have seen sterile neutrinos.
Online
sciencemag.org
Podcast interview  
          with author 
Adrian Cho.
The Sterile Neutrino: 
Fertile Concept or 
Dead End?
Dozens of physicists gathered recently to debate 
whether the phantom particle exists
 and if its worth hunting it
NEWSFOCUS
*
Sterile Neutrinos at the Crossroads, 2628 September.
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  305
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physics assumes that neutrinos are massless, 
but  most  extensions  of  the  theory  that  fix 
that problem include sterile neutrinos, says 
Paul Langacker, a theorist at the Institute for 
Advanced Study in Princeton, New Jersey. 
The sterile neutrino is not something bizarre 
or exotic, he says.
The details involve another key fact: As 
far as physicists know, all neutrinos spiral to 
the left, like footballs thrown by left-handed 
quarterbacks,  and  all  antineutrinos  spiral 
to the right. That would be ne if neutrinos 
traveled at unobtainable light speed. But as 
neutrinos  have  mass  and  travel  slower,  its 
possible in principle for an observer to over-
take a left-handed neutrino. The neu-
trino would then appear to travel 
the  opposite  way,  as  a  right-
handed  neutrinoa  particle 
not found in nature.
Theorists have found two 
ways  around  this  problem. 
First, when overtaken, an ordi-
nary left-handed neutrino could 
appear  instead  as  a  heavy  right-
handed sterile neutrino. Or second, the 
overtaken neutrino could appear as a right-
handed antineutrino. Even then, a theoreti-
cal seesaw mechanism would require heavy 
sterile neutrinos to explain why ordinary neu-
trinos are so light.
Thats plenty of reason to think sterile neu-
trinos are out there. However, most theories 
assume that sterile neutrinos are far heavier 
than ordinary neutrinos. For that reason and 
others, theory doesnt generally allow an ordi-
nary neutrino to just morph into a sterile neu-
trino in the way some experiments indicate, 
Langacker says. So its not clear that theorists 
and experimenters are stalking the same beast. 
Evidence of all sorts
The strongest experimental evidence for ster-
ile neutrinos comes from the Liquid Scintil-
lator Neutrino Detector (LSND), which ran 
at Los Alamos National Laboratory in New 
Mexico from 1993 through 1998. Using a par-
ticle accelerator, physicists generated muon 
antineutrinos that streamed through a detector 
lled with 167 tons of mineral oil.
Those  low-energy  muon  antineutrinos 
should have passed right through. However, 
an electron antineutrino could interact with 
the detector by merging with a proton to cre-
ate a positron and a neutronessentially, the 
weak  decay  of  the  neutron  run  backward. 
Thus,  physicists  could  spot  electron  anti-
neutrinos appearing in a beam of muon anti-
neutrinos. And they spotted 88 of them, give 
or take 23. Lo and behold, we saw an excess 
of events, says Los Alamoss William Louis.
Reported  in  1996  and  2001,  the  LSND 
results  might  seem  to  show  muon  anti-
neutrinos mixing into electron antineutrinos. 
But it couldnt be that simple, Louis says. Dif-
ferent avors of neutrinos mix at a rate that 
depends  on  the  difference  in  their  masses: 
The  bigger  the  mass  difference,  the  faster 
the mixing. Studies of atmospheric and solar 
neutrinos had placed limits on the mass dif-
ferences among the three neutrino avors, and 
the values were too low to explain the lickety-
split mixing that LSND saw as the particles 
ew just 30 meters, Louis says.
LSND  researchers  could  explain  their 
results, however, if muon antineutrinos oscil-
lated rst into sterile antineutrinos and then 
into electron antineutrinos. The sterile neu-
trinos would have to be heavier than ordinary 
neutrinos by 1 electron voltabout 100 times 
the differences among ordinary neutrinos.
Hints of extra neutrinos also come from 
the  heavens.  For  example,  cosmologists 
think the universe burst into existence in the 
big bang as an ultrahot, ultradense soup of 
particles. Tiny uctuations in the density of 
the soup then stretched to immense propor-
tions during a faster-than-light growth spurt 
known as ination and seeded the formation 
of galaxies. The uctuations also limit the 
number of neutrino types, theorist Kevork 
Abazajian of the University of California, 
Irvine, said at the meeting.
The density uctuations can be thought 
of as waves of various wavelengths randomly 
piled on one another. The uctuations inten-
sity  and  gravitational  pull  grow  stronger 
as  their  wavelengths  decreases;  then  the 
intensity peaks at a certain wavelength and 
starts to fall again. The position of that peak 
in  a  graph  of  intensity  versus  wavelength 
depends on the relative amounts of radiation 
and matter in the early universe. And because 
lightweight  neutrinos  acted  like  an  addi-
tional form of radiation, the position 
of the peak also reveals the number 
of types of light neutrinos.
To deduce the distribution 
and  the  peak  in  it,  scientists 
measure tiny variations in the 
afterglow of the big bangthe 
cosmic microwave background 
radiationacross  the  sky,  as 
NASAs  space-borne  Wilkinson 
Microwave Anisotropy Probe did from 
2001 to 2010. Scientists also measure the dis-
tribution of the galaxies, as the Sloan Digi-
tal Sky Survey has done using a telescope at 
the Apache Point Observatory in New Mex-
ico. The  results  suggest  a  fourth  neutrino, 
Abazajian says. Theres a 1-in-20 chance that 
its a statistical uctuation, and those sorts of 
things go away all the time, he says. Still, 
its intriguing that the datas converging to that 
value of four types of neutrinos.
The newest bit of evidence comes from 
nuclear reactors. Earlier this year, a team of 
theorists argued that reactors are putting out 
more  electron  antineutrinos  than  detectors 
tens of meters away show. The result suggests 
that some antineutrinos escape detection by 
morphing into sterile antineutrinos.
Within  a  nuclear  reactor,  nuclei  of 
the  isotopes  uranium-235,  uranium-238, 
plutonium-239,  and  plutonium-241  split 
randomly  to  make  myriad  smaller  nuclei 
that  release  copious  antineutrinos.  For 
example, a uranium-235 nucleus can split to 
make a nucleus of krypton-89. Krypton-89 
then  changes  identity  to  rubidium-89, 
strontium-89, and yttrium-89, as one neu-
tron  after  another  in  the  nucleus  spits  out 
an  electron  and  an  antineutrino  and  turns 
into a proton. Thousands of other chains or 
branches of decays also occur.
David  Lhuillier  of  Frances Alternative 
Energies  and Atomic  Energy  Commission 
in  Saclay  and  colleagues  kept  track  of  all 
those branches in a new calculation. Previ-
ous calculations showed that a score of reactor 
Far out! Cosmic microwave background (top) and 
the map of the galaxies hint at an extra neutrino.
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  306
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measurements taken over decades observed 
97.6%,  give  or  take  2.4%,  of  the  expected 
antineutrino uxne agreement with the 
prediction.  With  the  new  calculation,  the 
measurements average 94.3%, plus or minus 
2.3%a signicant difference that suggests 
neutrinos are disappearing. Before, all the 
experiments were in agreement with the pre-
diction, Lhuillier says. Now everybody is 
below the prediction. Physicists say this sin-
gle result triggered the workshop.
The disparate hints are tantalizing, says 
Joseph Formaggio of the Massachusetts Insti-
tute  of Technology  in  Cambridge.  Whats 
nice is that these anomalies come from differ-
ent directions, he says.
Signs of discord
Each  clue  comes  with  caveats,  however. 
For  example,  starting  in 
2002,  physicists  tested 
the LSND result with the 
Mini-Booster  Neutrino 
Experiment (MiniBooNE) 
at  Fermi  National Accel-
erator Laboratory (Fermi-
lab)  in  Batavia,  Illinois. 
First, they red muon neu-
trinosinstead of LSNDs 
muon antineutrinos450 
meters  into  a  detector 
filled  with  800  tons  of 
mineral oil. In 2007, they 
saw signs of electron neu-
trinos  appearing  in  the 
muon neutrino beam, but 
with the wrong energy to 
mirror the process seen in LSND with anti-
neutrinos. The result dampened enthusiasm 
for sterile neutrinos.
But last year, the researchers reported that 
using muon antineutrinos, they see electron 
antineutrinos appearing as LSND did, albeit 
at lower statistical signicance. The excess 
in the MiniBooNE antineutrino data agrees 
beautifully with what you would expect from 
LSND, says Louis, who also works on Mini-
BooNE. But it also makes matters more com-
plicated. To explain why the effect appears 
only for antineutrinos, physicists need to add 
two sterile neutrinos to their theory.
The  cosmological  evidence  for  sterile 
neutrinos also comes with qualications, says 
Yvonne Wong of RWTH Aachen University 
in Germany. The unknown particles scien-
tists might be glimpsing in cosmic radiation 
are signicantly lighter than the sterile neu-
trinos hinted at by LSND and MiniBooNE. 
They arent even necessarily true neutrinos, 
Wong  says,  but  could  be  any  feebly  inter-
acting particle.
Even the newfound reactor anomaly has 
not bowled skeptics over. Petr Vogel, a theo-
rist at the California Institute of Technology in 
Pasadena, who worked on the original reactor 
calculations 30 years ago, says the new cal-
culations are undoubtedly more thorough and 
realistic than the old ones. However, they still 
leave out important details that might make 
the falloff in neutrinos less impressive, Vogel 
says. I think what has been done is state of the 
art, and the shift [in the prediction] looks rea-
sonable to me, Vogel says. But whether the 
error is really 2.3% remains to be seen.
Finally, the signs of sterile neutrinos may 
not  agree  with  one  another,  says  Thomas 
Schwetz-Mangold of the Max Planck Institute 
for Nuclear Physics in Heidelberg, Germany, 
who presented a global t to all the data. In 
particular, if ordinary neutrinos quickly oscil-
late into sterile neutrinos, then experiments 
that send muon neutrinos to distant detectors 
should see a decrease in the total number of 
neutrinos reaching their detectors. But experi-
ments such as Fermilabs Main Injector Neu-
trino Oscillation Search, which res neutrinos 
735 kilometers to a detector in Minnesota, see 
no such loss. If I take everything at face value, 
then the probability is less than a percent that it 
all ts together, Schwetz-Mangold says.
The killer experiment
In spite of the odds, some experimenters are 
still eager to hunt sterile neutrinos. Plans vary 
widely, but physicists generally agree on what 
a killer experiment must do. If ordinary neu-
trinos morph into sterile neutrinos and back, 
then the number of ordinary neutrinos in a 
beam should go up and down as the neutri-
nos y away from their source. So scientists 
would have to spot that spatial oscillation over 
tens of meters.
The easiest way would be to add a sec-
ond detector to the MiniBooNE experiment 
closer to the neutrino source or to move the 
existing detector. The rate at which electron 
antineutrinos  appear  should  then  change. 
Building a second detector 200 meters from 
the source would cost $10 million, Geoffrey 
Mills,  a  MiniBooNE  team  member  from 
Los Alamos, said at the conference. Alter-
natively, researchers could move the current 
detector for about $5 million, he reported.
Adding the second detector to MiniBooNE 
is  a  must-do,  some  researchers  say.  But 
Roxanne Guenette of Yale University warned 
that a denitive measurement would likely 
take two more-expensive new detectors.
Others want to look for the oscillation of 
electron neutrinos by putting an intense radio-
active  source  inside  a  jumbo  detector. The 
number of electron neutrino detections should 
go  up  and  down  as  the  distance  within  the 
detector  from  the  source 
increases. Virginia Techs 
Jonathan  Link  proposes 
placing  a  chromium-51 
source in the center of the 
Sudbury Neutrino Obser-
vatory, which is a sphere 
filled  with  1000  tons  of 
heavy water.
The source should cost 
less than $3 million, Link 
says. I do believe that this 
is the cheapest option that 
has some chance of mak-
ing some sort of statement 
about the LSND-type ster-
ile neutrino, he says. Gio-
acchino Ranucci of Italys 
National Institute of Nuclear Physics in Milan 
presented a proposal to place a source under 
the 270-ton Borexino detector in Italys sub-
terranean Gran Sasso National Laboratory.
Hanging over all of this is the question of 
money,  as  the  United  States  particle  phys-
ics budget has been stuck at $800 million for 
years. Virginia Techs Ramaswamy Raghavan 
is developing the Low Energy Solar Neutrino 
Spectrometer  detector,  which  would  study 
solar neutrinos and, with a radioactive source, 
could look for sterile neutrinos. It would cost 
$50 million to $75 million. Can you predict 
in the current scal situation in the U.S. that 
this is going to happen? Raghavan says.
To help make the case for funding, con-
ference attendees plan to write a white paper 
laying out the options. Theres some urgency, 
says  Huber,  the Virginia Tech  theorist  who 
helped organize the meeting. I dont want to 
do sterile neutrinos my whole career, he says. 
He doesnt say whether the ephemeral beast 
will  continue  to  entice  him  if  no  denitive 
answer is quick in coming.  ADRIAN CHO
MIA. New calculations suggest that nuclear reactors 
put out more neutrinos than are observed.
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  307
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Its a problem that all social scientists face. 
You have a brilliant idea for a study. You have 
the experimental design all worked out, and 
your universitys review board has approved 
it. But you still have to recruit hundreds of 
people as subjects for the experiment.
Gabriel Lenz, a political scientist at the 
University of California, Berkeley, faced this 
problem last year when he and collaborators 
wanted to follow up on another groups study 
of voting behavior (Science, 10 June 2005, 
p.  1623).  For  that  study,  Americans  were 
shown photographs of past U.S. congressional 
candidates and asked to rate the politicians on 
various characteristics, such as competence 
and  attractiveness.  Even  though  the  study 
subjects had no information beyond an image 
of the candidates faces, their snap judgments 
were a signicant predictor of who actually 
won the races. Lenz wanted to see if that sur-
prising result collapsed when those evaluating 
the photos come from cultures different from 
those of the candidates. But how to recruit 
people living in multiple countries? 
Lenz and his research assistant Michael 
Myers had an idea: Why not order research 
subjects through Amazon.com? The company 
runs an online marketplace called Mechani-
cal Turk for people across the world avail-
able to do work on computers. (The name is 
a reference to an 18th century chess-playing 
machine that actually worked by virtue of 
a man hidden inside.) For tiny sums, anyone 
can hire people to perform almost any kind of 
simple task, such as tagging items in images. 
Lenzs experiment required people to look at 
photographs of Brazilian political candidates 
and ll in a data sheet.
But  first,  he  and  his  colleagues  had  to 
decide  on  how  much  they  would  pay  each 
participant.  Those  offering  a  job  through 
MTurk, known as requestors, compete with 
each  other  to  recruit Turkers,  the  500,000 
people currently registered with the MTurk 
site as available for work. The task of rating 
the political candidate photos required about 
4 minutes. We played around with various 
payment rates, Lenz says. For Turkers based 
in India, the researchers started low, offering 
15 cents. In just 4 days, they received data 
from 100 people. Then for a control group, 
they recruited more than 300 Americans for 
between 20 and 50 cents each. The total cost? 
About $160, and that includes the 10% fee 
Amazon charges.
In just a few weeks, Lenz had all the data 
his group needed. In spite of the cultural dif-
ferences, the snap-judgment effect persisted: 
American and Indian subjects predicted the 
winners of Brazilian political races based on 
nothing more than a mug shot, the research-
ers  reported  last  year  in  the  social  science 
journal World Politics.
As others follow Lenzs lead, many more 
social science papers using MTurk will appear 
in the coming years, predicts Adam Berinsky, 
a political scientist at the Massachusetts Insti-
tute of Technology in Cambridge. Everyone I 
know is using it, he says. For example, social 
scientists used 10,000 Turkers to create a tool 
for tracking the emotional content of Twitter 
messages (Science, 30 September, p. 1814).
For now, most researchers are using MTurk 
for pilot studies, quickly and cheaply testing 
online versions of experiments that they then 
perform with subjects face to face. But the 
use of MTurk subjects will eventually become 
mainstream,  Berinsky  says.  The  obvious 
advantage is the speed and cost. Generally, 
we pay $8 for a 15- to 20-minute experiment 
in a lab. We can run the same study on MTurk 
for 75 cents to a dollar.
There  are  other  advantages.  Turkers 
are amazingly focused research subjects, 
Berinsky  says.  Unlike  the  typical  univer-
sity undergraduates used for social science 
studies, Turkers get paid only if they 
generate  usable  data. This  is  neces-
sary to eliminate not only people who 
dont  understand  the  task  but  also 
spammers, people who try to exploit 
MTurk by skimming through the jobs 
and giving random responses wherever 
possible to accelerate the process. 
For  example,  Lenz  had  to  reject 
about 20% of his American and 50% 
of  his  Indian  Turkers  for  those  rea-
sons.  But  that  is  a  manageable  problem, 
Berinsky says. A counterintuitive solution is 
to keep the price low. If you offer more than a 
dollar, you attract the spammers who sort jobs 
by level of pay, he says. You have to nd the 
sweet spot where the payment is not too high 
but still attractive enough for most Turkers. 
So far, that sweet spot seems to be between 
15 and 50 cents for a 10-minute job.
Even if MTurk is cheap and fast, doubts 
will  linger  about  interpreting  data  from 
research subjects whom you never meet. To 
address those concerns, Berinsky and Lenz 
are teaming up with Gregory Huber, a politi-
cal scientist at Yale University, to study the 
Turker population. And of course, they are 
using MTurk to do so. They recently repli-
cated two classic survey experiments and a 
political science experiment. In each case, 
the data obtained with MTurk were consis-
tent with published studies that tested people 
in laboratories. 
The  scientists  have  found  some  differ-
ences,  too. Turkers  are  younger  and  more 
ideologically  liberal  than  the  U.S.  public, 
Berinsky says. However, they are more repre-
sentative of the U.S. population than a typical 
cohort of university undergraduates.
There  is  one  long-term  concern:  the 
super-Turkers, people who are essentially 
professional workers on MTurk, some of them 
logging more than 20 hours per week. Many 
social science experiments rely on the sub-
jects not knowing the researchers intentions. 
Berinsky says super-Turkers could potentially 
skew experiments if they try too hard to please 
researchers.  There  is  incentive  to  do  that 
because MTurk uses a reputation system. If a 
Turker does not have at least a 95% positive 
approval rating from their requestors, theyll 
often go unhired. 
Mechanical Turk seems like the prover-
bial goose that lays the golden eggs, Berinsky 
says. But I worry that in the rush for cheap 
research subjects, were going to trample the 
goose to death.  JOHN BOHANNON
Global pool. This map shows a 10% sample 
of workers (red) available on Amazon.coms 
Mechanical Turk.
Social scientists are turning to online retail giant Amazon.com to cheaply recruit 
people around the world for research studies
Social Science for Pennies
HUMAN  SUBJECT  RESEARCH
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  308
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In 2005, a handful of young researchers in 
Santa Barbara, California, were fed up with 
their inability to answer a major ecological 
question by reviewing the literature. So they 
decided to take matters into their own hands 
and created a network of small experiments. 
In the past 6 years, the network has spread 
to six continents and is now poised to make 
substantial contributions to ecology. Were 
on  the  edge  of  something  big,  says  John 
Orrock of the University of Wisconsin, Mad-
ison, a network co-founder.
The half-dozen Ph.D. students and post-
docs were part of a workshop at the National 
Center for Ecological Analysis and Synthesis 
(NCEAS) in Santa Barbara. The group was 
investigating fundamental inuences on the 
structure of grasslands, 
such  as  herbivory  and 
nutrients. Trying to ana-
lyze data from far-ung 
places,  the  group  was 
stymied  by  a  common 
obstacle.  Its  really 
fr ustrating  because 
everyone  does  their 
studies differently, says 
Elizabeth Borer, who is 
now at the University of 
Minnesota, Twin Cities. 
During  a  coffee 
break at NCEAS, Borer 
and a few others hatched a plan: They would 
each set up a small research plot, use the same 
methods, then pool their data. The vision was 
a network of sites that would be quick and 
cheap to set up without the need for major 
grants, enabling simple experiments around 
the world. Its like big science on a shoe-
string, says Scott Collins of the University 
of  New  Mexico,  Albuquerque,  who  later 
joined the network.
The  collaboration,  called  the  Nutrient 
Networknow  known  as  NutNethas 
grown far beyond initial expectations, with 
scientists volunteering at 68 sites in 12 coun-
tries. In part, its popular because the simple 
experiments are designed to answer a broad 
set of questions about how grasslands respond 
to global changewithout disproportionate 
effort by any one individual. Its not a brand-
new idea, but its novel that theyve pulled it 
off, says Alan Townsend of the University of 
Colorado, Boulder, who is not involved. The 
network also provides an easy way for young 
faculty members, postdocs, and grad students 
to get involved in a large collaboration and 
contribute to high-prole papers. 
So far, the effort has been funded with 
just a single $322,000 grant from the U.S. 
National Science Foundation (NSF) for coor-
dinating data and analysis, yet already the 
rst few papers have been published over the 
past year. The most recent, which appeared in 
Science last month (23 September, p. 1750), 
challenged a long-standing idea in ecology 
about plant diversity and productivity. Doz-
ens more papers are in the works, and ecol-
ogists enthuse about the networks potential 
for cost-effective, rapid results. NutNet has 
tremendously  improved  on  the  way  weve 
done things, says Alan Knapp of Colorado 
State University, Fort Collins, another ecolo-
gist who is not involved. Ive been incred-
ibly impressed.
Keep it simple
Research networks arent new to ecology, of 
course. The Long Term Ecological Research 
(LTER) network, for example, is composed 
of 26 research sites and stations, almost all in 
the United States, that have been collecting 
data for 30 years. And construction began 
this fall on some of the 20 U.S. observatories 
that will make up the $434 million National 
Ecological Observatory 
Network.  These  hefty 
networks require a fair 
amount  of  money  to 
operate,  because  staff 
members  collect  hun-
dreds of types of data, 
often year-round. 
During the NCEAS 
workshop,  NutNets 
f ounde r s   qui c kl y 
sketched an alternative 
vision: Each researcher 
would  conduct  the 
same  few  experiments 
Open-Source Ecology Takes Root 
Across the World
A new collaboration of volunteer research sites is running simple yet powerful 
experiments to shed light on global change in grasslands
NETWORK  SCI ENCE   
Experimental
Observational
only
Diversity. NutNet sites include 1747 plant taxa in many ecosystems, such as (see photos, left 
to right) subalpine grassland, alpine meadow, desert, pasture, sagebrush steppe, and savanna.
Standardized. Researchers worldwide add nutri-
ents and measure plots the same way.  
China
Australia
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011  309
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in several plots of 25 square meters. They 
would  add  combinations  of  three  crucial 
plant nutrientsnitrogen, phosphorus, and 
potassiumand  they  would  fence  part  of 
the plots to exclude deer, zebras, kangaroos, 
and other herbivores. 
By measuring changes in biomass and spe-
cies composition, they would try to tease apart 
the relative impact of herbivores and nutrients 
on  the  structure  of  the  com-
munity. Ecologists have been 
fascinated  by  this  question 
for a long time, Orrock says. 
Moreover,  the  experiments 
simulate the impacts of anthro-
pogenic global change. Nutri-
ent  levels  have  been  boosted 
dramatically by fertilizers and 
pollution from fossil fuels. At 
the  same  time,  humans  have 
altered  the  density  of  herbi-
vores in many places through 
farming or indirectly by hunt-
ing of predators.  
Several  attendees  at  the 
NCEAS  workshop  immedi-
ately  volunteered  to  partici-
pate. One of the rst was Helmut Hillebrand 
of the Carl von Ossietzky University of Old-
enburg  in  Germany,  who  set  up  a  NutNet 
site, even though hes a plankton ecologist. 
I think its the next generation of ecologi-
cal experiments, he says. The site he started 
is located in an old eld 5 minutes from his 
parents house, so he drops by to collect data 
while visiting. 
Borer and the others also invited a few 
colleagues  to  join,  and  the  idea  began  to 
spread by word of mouth. Sensing potential, 
the group sent an e-mail in November 2006 
to just about every grassland ecologist they 
knew. By the time data started arriving the 
next year, there were 51 sites.
Members of the network agree to submit 
data immediately to a central database. All 
participantsnow  about  100,  including  a 
dozen or so graduate studentshave access 
to the data. Simply by contributing data, they 
can be an author on high-prole papers that 
address the projects big questions. The net-
work is already making a mark: Last months 
paper  in  Science  showed  that  a  textbook 
idea  about  the  relationship  between  plant 
productivity  and  species  richness  in  fact 
occurs rarely. Other key papers, based on the 
experimental results of adding nutrients and 
excluding herbivores, are still being written. 
NutNet participants must propose papers 
on  additional  ideas  to  the  whole  group. 
The goal is to avoid duplication and allow 
other members to contribute to analysis or 
writing  the  manuscript.  Jennifer  Firn  of 
the  Queensland  University  of Technology 
in  Brisbane,  Australia,  for 
example,  wanted  to  look  at 
invasive species in the plots. 
The process of turning this 
idea into a paper was the best 
learning  experience  I  have 
ever  had,  says  Firn,  who 
became an assistant professor 
in February. I had more than 
30  authors  and  co-authors, 
so  it  meant  so  much  advice 
and expertise were available. 
Published in Ecology Letters
in March, the paper showed 
that non-native plants, some 
invasive,  dont  all  spread 
like the worst weeds. Instead, 
most  species  in  the  NutNet 
plots  were  about  as  common  in  their  new 
environment as in their native range. That 
suggests  that  regulators  of  plant  imports 
might want to focus on screen-
ing out plants that are highly 
abundant overseas. 
Network  members  decide 
among themselves what kinds 
of  additional  data  to  gather. 
This  is  like  an  indie  garage 
band,  a  cooperative  without 
all the top-down headaches, 
says  co-founder  W.  Stanley 
Harpole,  an  assistant  pro-
fessor  at  Iowa  State  Univer-
sity  in  Ames.  (Others  make 
analogies to the development 
of  open-source  software  or 
start-up companies.) Eighteen 
members are analyzing regular 
deliveries from other participants, who col-
lect everything from soil microbes to arthro-
pods and leaf litter. It is simple, mail-order 
sampling, says co-founder Eric Seabloom 
of the University of Minnesota, Twin Cities. 
The person in the eld doesnt have to do 
that much.
Facing the future
An all-volunteer approach may have its limi-
tations, however. So far, the majority of sites 
are in the United States. Peter Adler of Utah 
State University in Logan, a co-founder, says 
the group tried to recruit scientists in South 
America without much success. Maybe its 
just [bad] luck, he says. Townsend expects 
that more researchers in less developed coun-
tries will eventually sign up, as word spreads 
about the network and its publications. Ear-
lier this month, several sites in India agreed 
to  provide  observational  data,  and  a  few 
more will also conduct experiments. 
A larger question is how long a volun-
teer effort can be sustained. In absence of 
external funding, I fear that the good will of 
those individuals and their institutions may 
not persist, says Michael Willig of the Uni-
versity of Connecticut, Storrs, who is not a 
participant in the network. But co-founder 
Melinda Smith of Yale University predicts 
that  interest  will  remain  high  as  long  as 
the network produces high-impact papers. 
Harpole points out that each plot has space 
reserved  for  experiments  not  yet  planned. 
Were banking for the future, he says.
The  looming  danger  is  the  expiration 
of  the  NSF  grant  in  January  2013. These 
funds  pay  for  collaboration  meetings  and 
for  a  postdoc,  Eric  Lind  of 
the  University  of  Minnesota, 
Twin Cities, who runs the cen-
tral  database.  The  death  of 
the Nutrient Network will be 
when the funding for that post-
doc position runs out, Adler 
says. The steering committee 
hopes to cover those expenses 
with future research grants for 
more ambitious analyses. 
Even if the NutNet peters 
out, the founders hope it will 
be a model. To Borer, the suc-
cess so far shows that individ-
ual  scientists  at  any  stage  of 
their  career  can  help  answer 
big questions even if they havent landed a 
major grant. Were out to change the cul-
ture, she says. The success of this model 
could  empower  other  groups  to  address 
equally important ecological problems at a 
global scale.
ERIK STOKSTAD
Were out to 
change the culture.
ELIZABETH BORER,
UNIVERSITY OF MINNESOTA,
TWIN CITIES
This is like an indie 
garage band.
STAN HARPOLE,
IOWA STATE UNIVERSITY
USA   USA Switzerland   Tanzania
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  310
LETTERS
edited by Jennifer Sills
LETTERS  I  BOOKS  I  POLICY FORUM  I  EDUCATION FORUM  I  PERSPECTIVES
312
A multiple personality fable
Bending light with 
antenna arrays
317
COMMENTARY
Martial Arts Research: 
Prudent Skepticism 
A.   DI AMOND  AND  K.   LEE S  REVI EW 
Interventions shown to aid executive func-
tion development in children 4 to 12 years 
old (special section on Investing Early in 
Education,  19 August,  p.  959)  leaves  the 
impression that martial arts training as usu-
ally delivered enhances executive functions. 
This  is  far  from  established.  Martial  arts 
training is a heterogeneous independent vari-
able with average effects that may be negli-
gible or even negative.  
Diamond and Lee cite two studies in sup-
port of martial arts. In the Trulson study (which 
was based on 34 students and 1 instructor), 
the only outcome measures are the self-report 
personality  inventories  completed  by  the 
delinquent students (1). Trulson concluded 
that the meditation, contemplation of goals, 
and other noncombat components of martial 
arts are helpful, but pure competitive ght 
training is harmful. The Lake and Hoyt study 
(207 students and 1 instructor) found the most 
positive effects on a measure of behavior dur-
ing completion of an obstacle course (2). With 
teacher ratings, however, insignicant effects 
were reported for four out of ve variables, 
including self-control.
Longitudinal studies observing the results 
of many instructors lead to skepticism about 
the effects of martial arts training. Endresen 
and Olweus (3), using a longitudinal design, 
reported that participation in power sports 
Editorial Expression of Concern
IN THE 4 JUNE 2010 ISSUE, SCIENCE PUBLISHED THE REPORT SPHK1 REGULATES PROINFLAM-
matory responses associated with endotoxin and polymicrobial sepsis by P. Puneet et al. (1). 
After the receipt of an anonymous e-mail on 22 March 2011, Science learned that authori-
ties at the authors principal institutions at the time of publication (University of Glasgow 
and National University of Singapore) and the University of Liverpool (corresponding author 
A.J.M.s more recent afliation) were investigating allegations of gure manipulation in the 
Science Report and in a paper published in Nature Immunology [Nature Immunology 12, 344 
(2011)] also by P. Puneet et al. The Nature Immunology paper was subsequently retracted after 
an investigation by the University of Liverpool, but we have been informed that the investiga-
tion into the Science Report has not yet reached a conclusion, despite indications that it was 
near completion.
On 14 January 2011, Science published a Correction to two of the gures in the Puneet et 
al. Report, after correspondence with A.J.M. In light of the continuing investigation, we can no 
longer be condent in the reliability of the corrected record. Pending the results of the investiga-
tions, Science is publishing this Editorial Expression of Concern to alert our readers to the fact 
that serious questions have been raised about the validity of ndings in the Puneet et al. paper.
BRUCE ALBERTS
 Editor-in-Chief
Reference
  1.  P. Puneet, C. T. Yap, L. Wong, L. Yulin, D. R. Koh, S. Moochhala, J. Pfeilschifter, A. Huwiler, A. J. Melendez, Science 328, 1290 
(2010).
    Published online 3 October 2011; 10.1126/science.1214735
[including martial arts] actually leads to an 
increase or enhancement of antisocial involve-
ment in the form of elevated levels of violent 
as well as non-violent antisocial behavior out-
side sports. We analyzed data from a large, 
nationally representative sample (4). The out-
come  variable  was  teacher-rated  behavior, 
including self-control and attention. In each of 
our two main outcome analyses, we found that 
martial arts had no effect on behavior.  
In a world beset by violence, there is irony 
and pathos in hoping that our children will be 
improved by teaching punching, kicking, and 
tripping. Unless the evidence for benet is 
robust, it is prudent to be skeptical.
JOSEPH M. STRAYHORN
1
* AND 
JILLIAN C. STRAYHORN
2
1
Department  of  Psychiatry,  Drexel  University  College  of 
Medicine, Philadelphia, PA 19129, USA. 
2
Undergraduate, 
Department of Psychology, Cornell University, Ithaca, NY 
14853, USA.
*To whom correspondence should be addressed. E-mail: 
joestrayhorn@gmail.com
References
  1.  M. E. Trulson, Hum. Relat. 39, 1131 (1986).
  2.  K. D. Lakes, W. T. Hoyt, Appl. Dev. Psychol. 25, 283 (2004).
  3.  I. M. Endresen, D. Olweus, J. Child Psychol. Psych. 46, 
468 (2005).
  4.  J. M. Strayhorn, J. C. Strayhorn, J. Child Adolesc. Psychiatr. 
Ment. Health 3, 32 (2009).
Martial Arts Research: 
Weak Evidence
THE  REVIEW  INTERVENTIONS  SHOWN  TO 
aid executive function development in chil-
dren 4 to 12 years old by A. Diamond and 
K. Lee (special section on Investing Early in 
Education, 19 August, p. 959) cited work that 
close examination shows to be weak. Some of 
the studies (1, 2) were randomized, but they 
failed  to  meet  other  criteria  such  as  blind-
ing of teachers and parents to pupils treat-
ment groups. Studies involving martial arts 
and physical exercise were particularly weak 
on isolation of variables. One study on mar-
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   311
318   321
Signs of ocean 
eddies
Information capacity 
in cell signaling
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tial  arts  training  for 
children  (1)  com-
pared  a  treatment 
group who wore spe-
cial uniforms, medi-
tated, bowed to their 
instructor,  and  were 
reminded  of  self-
awareness  and  self-
control,  to  a  control 
group who continued 
with  their  ordinary 
physical  education 
activities; these authors concluded that when 
some improvement on some scales occurred 
for  the  treatment  group,  the  change  was 
caused by the self-awareness and self-control 
messages, rather than by other ways the two 
groups differed. Another study (2) compared 
children who did sport stacking, a bimanual 
physical task, with a control group that did not 
experience any exciting new activity, and con-
cluded that improvement on one of two read-
ing measures was caused by the stacking task. 
A relevant volume dealing with treatments 
for developmental disabilities (3) stressed the 
weakness of evidence for special education 
interventions and described some such con-
ditions as fad magnets. Unfortunately, early 
educational interventions seem to be similarly 
weak in evidence. The stakes are high and the 
resources scarce in both cases.  JEAN MERCER
Richard Stockton College, Pomona, NJ 08240, USA. E-mail: 
jean.mercer@stockton.edu
References
  1.  K. D. Lakes, W. T. Hoyt, Appl. Dev. Psychol. 25, 283 (2004).
  2.   T. A. Uhrich, R. L. Swalm, Percept. Mot. Skills 104, 1935 
(2007).
  3.  J. W. Jacobson, R. M. Foxx, J. A. Mulick, Controversial 
Therapies for Developmental Disabilities (Erlbaum, 
Mahwah, NJ, 2005).
Response
WE AGREE WITH STRAYHORN AND STRAYHORN 
that modern and traditional versions of mar-
tial  arts  differ. We  tried  to  emphasize  that 
modern American martial arts (which empha-
size punching and kicking and competi-
tion) have been found to make unproductive 
behaviors worse, whereas evidence indicates 
that traditional martial arts [which emphasize 
self-control, self-defense, patience, waiting 
for the other person to make an error, con-
centration, respect, and humility (1)] improve 
executive functions.  
We agree with Mercer about weaknesses 
in many studies thus far published on execu-
tive function interventions. We reviewed only 
peer-reviewed studies and provided detailed 
information about them (see tables S1 to S3 in 
the supporting online material) to give read-
ers an opportunity to judge the evidence for 
themselves. We disagree with Mercer about 
the martial arts study being particularly weak. 
First studies are designed to determine whether 
there is an overall difference. Follow-up stud-
ies can then try to dissect which aspect(s) of 
a program had the most effect. That said, the 
martial arts study by Lakes and Hoyt (1) is to 
be commended. It used random assignment, 
pre- and post-testing, an intervention imple-
mented during regular school hours (making 
it feasible to reach many children), an active 
control group that also engaged in physical 
activity, and incrementally increasing levels 
of difculty in the martial arts condition, and 
it provided evidence that executive-function 
improvements generalized to multiple con-
texts. Unlike many studies that have targeted 
disadvantaged children and/or those behind 
on executive function, children in this study 
were socioeconomically advantaged, making 
the ndings especially impressive.   
ADELE DIAMOND* AND KATHLEEN LEE
Department  of  Developmental  Cognitive  Neuroscience, 
University of British Columbia, Vancouver, BC V6N 3L6, BC, 
Canada.
*To whom correspondence should be addressed. E-mail: 
adele.diamond@ubc.ca
Reference
  1.  K. D. Lakes, W. T. Hoyt, Appl. Dev. Psychol. 25, 283 
(2004).
Letters to the Editor
Letters (~300 words) discuss material published in 
Science in the past 3 months or matters of gen-
eral interest. Letters are not acknowledged upon 
receipt. Whether published in full or in part, Let-
ters are subject to editing for clarity and space. 
Letters submitted, published, or posted elsewhere, 
in print or online, will be disqualied. To submit a 
Letter, go to www.submit2science.org.
CORRECTIONS AND CLARIFICATIONS
Review: Interventions shown to aid executive 
function development in children 4 to 12 years 
old by A. Diamond and K. Lee (special section 
on Investing Early in Education, 19 August, p. 
959). The journal cited in reference 28 should 
have been Appl. Dev. Psychol.
Education  Forum:  Mathematics  teachers 
subtle,  complex  disciplinary  knowledge  by 
B. Davis (24 June, p. 1506). The number line 
on  the  right  in  part  C  of  the  gure  was  mis-
numbered. The correct panel is shown here.
TECHNICAL COMMENT ABSTRACTS
Comment on How Cats Lap: Water Uptake by Felis catus
Michael Nauenberg
Reis et al. (Reports, 26 November 2010, p. 1231) reported on the mechanism by which cats lap and gave a theo-
retical and experimental analysis of their observations. Their explanation for the cats lapping frequency, however, 
is based on an incorrect application of the principles of uid dynamics. The revised analysis given here agrees with 
their observations and predicts a similar lapping frequency for cats and dogs.
Full text at www.sciencemag.org/cgi/content/full/334/6054/311-b
Response to Comment on How Cats Lap: Water Uptake by Felis catus
Roman Stocker, Jeffrey M. Aristoff, Sunghwan Jung, Pedro M. Reis
We return to the physics of cat lapping to show that our proposed scaling analysis predicts the functional depen-
dencies revealed by the experimental data more accurately than a recently proposed alternative description by 
Nauenberg. Experimental verication of functional dependencies, rather than single numerical values, represents 
the appropriate test for any scaling argument.
Full text at www.sciencemag.org/cgi/content/full/334/6054/311-c
C
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Factor a (multiplier):
adjustment ratio
Factor b (multiplicand):
starting position
Product c:
corresponding position
on the adjusted number 
line
BOOKS ET AL.
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n 1972, incorporation papers for Sybil, 
Incorporated, were drawn up by a patient, 
her therapist, and a journalist who had 
just nished writing a book about her case. 
Flora Rheta Schreibers Sybil 
( 1) told the story of a young 
woman  who  was  cured  of 
having  her  consciousness 
split into 16 separate person-
alities. The corporations pur-
pose was to share the prots 
from the book, a planned lm, 
and  spin-offs  that  included 
T-shirts,  dolls,  a  jigsaw 
puzzle,  and  a  board  game. 
Although  the  corporation 
did not last and the ancillary 
products did not materialize, the book sold 
millions of copies. It was dramatized twice 
in made-for-television movies. In the rst, 
Sybils  psychiatrist  was  played  by  Joanne 
Woodward,  who  had  previously  won  the 
Academy Award for Best Actress for her per-
formance in the role of a patient with mul-
tiple personality disorder in Nunnally John-
sons 1957 lm The Three Faces of Eve.
The most notable product of Sybil, Inc.s 
principals  was  the  epidemic  of  multiple 
personality disorder that swept the United 
States in the 1970s and 1980s. Unlike most 
previous  cases,  these  late-20th-century 
variants  featured  personalities  stuck  in 
various stages of childhood. The patients 
alters  revealed  memories  of  childhood 
sexual  abuseoften  horricelicited  by 
hypnosis. Today, researchers and clinicians 
are skeptical about most cases of multiple 
personality disorder, which has been recon-
ceptualized and renamed dissociative iden-
tity disorder.
Over  the  past  two  decades,  revelations 
have  emerged  to  raise  doubts  about  the 
validity of the case of Sybil. First, a clinician 
who had met the patient disputed the diag-
nosis promoted in the book. Then, tapes left 
by the books author suggested that she col-
luded with the therapist to create symptoms 
to t their diagnosis.
In  Sybil  Exposed,  journalist  Debbie 
Nathan chronicles the rise and fall of Sybil 
as the paradigm-setting case of multiple per-
sonality disorder. She does so in three inter-
twined biographies, beginning with that of 
the patient, Shirley Mason. Masons upbring-
ing  was  strict  (Seventh  Day 
Adventist), and although her 
mother was odd and subject 
to mood swings, she was not 
the  sexual  sadist  depicted 
in  Sybil.  Starting  at  age  22, 
Mason was treated by Corne-
lia Wilbur, an ambitious psy-
chiatrist who progressed from 
treating  traumatized  World 
War II soldiers with hypno-
sis  and  sodium  pentothal  to 
inducing traumatic memories 
in Mason with the same tools. This she did 
on and off for more than two decades, rst in 
Nebraska and then in New York City. In New 
York, Wilbur often saw Mason daily, making 
house calls in the evening with a satchel of 
drugs and a portable electroconvulsive ther-
apy machine. Beginning in 1963, the patient 
and her therapist collaborated with Schreiber, 
a journalist with a tendency to make her mag-
azine stories more salable by massaging bio-
graphical details.
Nathan  offers  a  compelling  account  of 
the creation, packaging, and selling of this 
case of medical and journalistic malpractice. 
Her sources include transcripts of therapy 
sessions, letters by the patient to childhood 
friends  and  former  roommates,  and  inter-
views with acquaintances and colleagues of 
all three women. Nathans credentials suit 
this  topic  well,  as  she  coauthored  an  ear-
lier book (  2) that helped reverse the ood 
of false memories implanted in children by 
prosecutors and therapists inspired by Sybil. 
As a feminist, she was dismayed that a seg-
ment of the womens movement channeled 
its social concerns into a hunt for psycho-
sexual demons that unjustly targeted teach-
ers and day care workers.
Analyzing  the  significance  of  Sybil, 
Nathan shows how the dilemmas faced by 
postWorld War II women helped shape that 
case and gave it cultural resonance. Wilbur, 
she  explains,  saw  herself  as  a  psychiatric 
Betty Friedan, encouraging female patients 
to try out new social roles and, indeed, even 
new  personalities.  Similarly,  journalist 
Schreiber saw Mason as a country girl from 
a stiing background who found a new iden-
tity in the big city. Both Wilbur and Schreiber 
had  struggled  to  find  acceptance  in  male-
dominated professions and reveled in the sta-
tus and remuneration that Sybil brought them.
Looking beyond the three women who 
created Sybil, Nathan explores the institu-
tional and professional context of both that 
case and the epidemic that followed. With 
its shifting boundaries and history of diag-
nostic uncertainty, psychiatry was a medi-
cal specialty with little resistance to the fad-
dishness  and  yearning  for  breakthroughs 
that fueled the multiple personality disor-
der fervor. Adding to clinicians enthusiasm 
was  the  embrace  of  multiple  personality 
disorder by celebrities, journalists, and tele-
vision producers.
In concluding her cautionary tale of this 
great American multiplicity, Nathan regrets 
that desire for personal change went awry at a 
fractured moment in history. The result was 
that women and their social struggles were 
reduced to a bizarre illness. The cure was not 
critical inquiry or protest marches or efforts 
at the polls. Instead the cure was drugs [and] 
hypnosis. Reading Sybil Exposed, that con-
clusion seems warranted. 
References
  1.  F. R. Schreiber, Sybil (Regnery, Chicago, 1973).
  2.  D. Nathan, M. R. Snedeker, Satans Silence: Ritual Abuse 
and the Making of a Modern American Witch Hunt (Basic, 
New York, 1995).
Sybil, Inc.
PSYCHIATRY
Ben Harris 
The reviewer is at the Department of Psychology, Univer-
sity of New Hampshire, Durham, NH 03824, USA. E-  mail: 
bh5@unh.edu.
Sybil Exposed
The Extraordinary Story 
Behind the Famous 
Multiple Personality Case
 by Debbie Nathan
Free Press (Simon and 
Schuster), New York, 2011. 
328 pp. $26, C$29.99, 16.95. 
ISBN 9781439168271.
10.1126/science.1212843
The  account  that  made  the  story  famous.  The 
cover of the rst edition of Sybil.
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   313
EDUCATIONFORUM
F
or academic researchers and educators, 
summer months are often among the 
most productive times of year. Unfortu-
nately, at many minority-serving institutions 
(MSIs) that serve a high proportion of under-
represented minorities (URMs), the summer 
often brings a brain drain that threatens to 
erode capacity for conducting research. Sum-
mer  research  programs  (SRPs)  recruit  stu-
dents from MSIs to spend a summer working 
at a research-intensive university. SRPs can 
expose students to resources and experiences 
they may not as easily access at their home 
MSI. Among  benefits  to  host  institutions, 
SRPs  help  fulfill  some  broader  impacts 
(i.e., nonresearch, such as education and out-
reach)  that  are  required  by  many  funders. 
MSI faculty may benet from skills the SRP 
students bring back. But this brain drain can 
undermine the ability of MSI faculty to effec-
tively teach research skills and to develop tal-
ent among a diverse pool of students.
In 2008, ~25% of U.S. science, technol-
ogy, engineering, and math (STEM) bacca-
laureate degrees awarded to URM students 
were from MSIs ( 1). These institutions enroll 
~30% of all URM students (  2). Although the 
percentage of URMs earning baccalaureate 
degrees has declined ( 1), those who complete 
their  degrees  show  Ph.D.  graduation  rates 
similar to non-Hispanic white counterparts 
( 1). Many MSIs are among the leading STEM 
bachelors  degreegranting  institutions  for 
Hispanic and African American students who 
complete  Ph.D.  degrees  ( 3).  But  whereas 
interest  in  diversity  underlies  undergradu-
ate SRPs, questions remain about intended 
recruitment and retention of URM students in 
graduate programs. Despite a steady increase 
in graduate program graduation rates over the 
past decades (  4), URM participation in STEM 
graduate programs is lower than expected on 
the basis of U.S. demographics ( 5).
Erosion of the Capacity to Develop Talent
Despite  SRPs  benefits,  they  may  hinder 
the ability of talented individuals to access 
the skill set required to succeed in research 
careers. Institutionalized one-way bridges, 
like SRPs, can siphon well-trained talented 
students  from  MSIs. As  a  result,  research 
goals of MSI faculty may not advance as well 
as they could; well-trained personnel are key 
to producing good-quality data that become 
the basis for publications and grant applica-
tions. In turn, reviews of research grant appli-
cations from MSIs may criticize productivity 
levels, the amount of preliminary data, and 
the adequacy of academic environments to 
implement research programs. Such percep-
tions of MSIs may erode funding for facili-
ties, equipment, and supplies.
A vicious cycle may unfold. Adequately 
supported  MSI  faculty  can  develop  talent 
among URM students with high potential, but 
lacking research experience. Early exposure 
to research ( 6) and long-term experiences (  6, 
 7) have been correlated with outcomes such 
as persistence in research careers. Applicant 
training is a key element in successful grant 
applications. Early and consistent access to 
research mentors and adequate resources may 
provide cumulative advantages (  8). Although 
it is not clear what factors contribute to differ-
ential success rates for URM faculty in obtain-
ing research funds (  8,   9), lack of funding in 
turn affects the overall capacity to develop and 
nurture local students, leading to a shortage of 
well-qualied, diverse talent.
Ensuring Long-Term Sustainability
Although  some  promising  programs  exist 
( 10), we must invest in sustainable develop-
ment of talent across a wider spectrum of aca-
demic institutions. This requires a shift away 
from the prevailing system at research-inten-
sive institutions ( 11) and MSIs ( 12) to provide 
research-intensive  experiences  for  all  stu-
dents. Collaborations between research-inten-
sive institutions and MSIs could be rebalanced 
for more two-way bridge partnerships.
For example, there are well-equipped MSI 
research  facilities  supported  by  initiatives 
from funders such as the National Institutes 
of Health and National Science Foundation 
(e.g.,  Spelman  Colleges  Center  for  Health 
Disparities Research and Education, and the 
Ponce School of MedicineMoffitt Cancer 
Center Partnership). Thoughtful integration 
of research and teaching training activities, 
guided by aligned interests, may allow a post-
doctoral fellow to receive training in teaching 
at a MSI partner school. Graduate students 
may gain valuable experience in communicat-
ing science ( 13) and acting as mentors to URM 
colleagues at partner MSIs. Students who act 
as role models demonstrate increased learn-
ing and tend to make stronger commitments 
to their studies (  14). Students from MSIs will 
share experiences with groups at SRP host 
institutions. This may increase their sense of 
belonging, shown to help students overcome 
the uncertainty ( 15) that discourages many 
from pursuing a STEM career ( 16).
The benets of diversity at all stages of 
the  academic  pipeline  ( 17)  are  well  docu-
mented  and  recognized  by  funding  agen-
cies ( 10). Amid calls for supporting MSIs to 
expand their effective recruiting and retention 
rates (  18), while establishing basic indicators 
of  student  outcomes  to  enable  institutions 
to assess their effectiveness ( 12), now is the 
time to rethink our approach to developing a 
diverse, talented STEM workforce.
References and Notes
  1.  National Science Foundation (NSF), Women, Minorities, 
and Persons with Disabilities in Science and Engineering: 
2011 (NSF, Arlington, VA, 2011).
  2.  X. Li, Characteristics of Minority-Serving Institutions and 
Minority Undergraduates Enrolled in These Institutions 
(NCES 2008-156, U.S. Department of Education, Wash-
ington, DC, 2007).
  3.  National Academies and Institute of Medicine, Expanding 
Underrepresented Minority Participation: Americas Science 
and Technology Talent at the Crossroads (National Acad-
emies Press, Washington, DC, 2010).
  4.  NSF, Doctorate Recipients from U.S. Universities: 2009 
(NSF, Arlington, VA, 2010); www.nsf.gov/statistics/
nsf11306.
  5.  P. Einaudi, Science Resources Statistics InfoBrief 
(NSF11-319, NSF, Arlington, VA, 2011).
  6.  S. H. Russell et al., Science 316, 548 (2007).  
  7.  A. L. Zydney et al., J. Eng. Educ. 91, 151 (2002).
  8.  D. K. Ginther et al., Science 333, 1015 (2011).  
  9.  L. A. Tabak, F. S. Collins, Science 333, 940 (2011).  
 10.  E. M. August et al., J. Cancer Educ.,  (2011); 10.1007/
s13187-011-0265-4.
 11.  W. A. Anderson et al., Science 331, 152 (2011).  
 12.  L. E. Malcom et al., Tapping HSI-STEM Funds to Improve 
Latina and Latino Access to the STEM Professions (Univ. 
of Southern California, Los Angeles, CA, 2010).
 13.  D. F. Feldon et al., Science 333, 1037 (2011).  
 14.  J. M. Good et al.,  J. Negro Educ. 69, 375 (2000).  
 15.  G. Cohen, J. Garca, Curr. Dir. Psychol. Sci. 17, 365 (2008). 
 16.  G. M. Walton, G. L. Cohen, J. Pers. Soc. Psychol. 92, 82 
(2007).  
 17.  P. Gurin et al., Harv. Educ. Rev. 72, 330 (2002).
 18.  E. M. Bensimon, L. E. Malcom, B. Dvila, (Re)constructing 
Hispanic-serving institutions: Moving beyond numbers 
toward student success (EP3: Education Policy and Prac-
tice Perspectives 6, Iowa State Univ., Ames, IA, 2010).
 19.  The author thanks undergraduate researchers (supported 
by Department of Defense grant W911NF-09-1-0219); 
particularly, D. Kiehart, T. Littleton, and C. Doe, who 
participated in the two-way collaboration. The author was 
supported by NSF. 
Rethink Summer Student Research
EDUCATION
Franklin A. Carrero-Martnez
Research and training at institutions serving 
minority students may suffer as top students 
leave for other schools each summer.
 Department  of  Biology,  University  of  Puerto  Rico, 
Mayagez,  Mayagez,  PR  00681,  USA.  E-mail:  franklin.
carrero@upr.edu  10.1126/science.1209555
AJournal withImpact fromAAAS, the publisher of Science
Science Translational Medicine
Integrating Medicine and Science
A recent journal article features the sequencing of fetal DNA from plasma
of a pregnant woman to permit prenatal, noninvasive genome-wide
screening to diagnose fetal genetic disorders.
Sci Transl Med 8 December 2010:
Vol. 2, Issue 61, p. 61ra91
DOI: 10.1126/scitranslmed.3001720
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In This Issue
Scientists   who   wish   to   pursue   academic   careers   in   Europe
have  much  with  which  to  contend,   especially  now  amidst   an
uncertain scal landscape. However, buttressed by the European
Commission,   several   member   states,   including  Germany,   the
United Kingdom, and France, as well as Scandinavia, have plans
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PERSPECTIVES
 E
lectrical  synapses  have  a  rich  and 
sometimes  controversial  history. 
During  the  early  20th  century,  the 
question of whether chemical or electrical 
synapses underlie the main mode of signal-
ing in the mammalian central nervous sys-
tem (CNS) was hotly debated (  1). However, 
after the discovery of neuronal inhibition in 
the early 1950s, it was accepted that trans-
mission of information via neurotransmit-
ter  molecules  (chemical  synapses)  repre-
sents  the  major  form  of  signaling  among 
CNS neurons. Although a consensus devel-
oped  that  electrical  synapses  are  present 
in a subset of neuronal connections, it was 
unknown  whether  these  synapses  exhibit 
selectivity and plasticity as shown for most 
chemical  synapses,  or  whether  neuronal 
activity can result in long-term change of 
synaptic strength of electrical synapses ( 2) 
in the mammalian CNS. On page 389 of this 
issue, Haas et al. (  3) demonstrate that the 
strength of electrical synapses among spe-
cic neurons in the thalamus of the mam-
malian brain affects long-term depression 
(LTD), a process important for learning and 
memory. Given the proposed role that elec-
trical synapses play in synchronizing neuro-
nal activity, these ndings suggest a mech-
anism  for  controlling  the  coordination  of 
neuronal activity.
Chemical  synapses  selectively  connect 
different types of neurons to provide a spe-
cific  path  of  communication  among  CNS 
neurons ( 4,   5). It was discovered more than 
10  years  ago  that  electrical  synapses  are 
formed  with  exquisite  selectivity  among 
specic classes of inhibitory neurons (  6,  7). 
Moreover, another hallmark of synapses
modulation by neurotransmittershas been 
also demonstrated in both the thalamus and 
hippocampus (  8,  9). 
To  investigate  the  effects  of  neuronal 
activity  on  the  strength  of  electrical  syn-
apses in the mammalian CNS, Haas et al. 
recorded  electrical  activity  from  pairs  of 
neurons in the rat thalamic reticular nucleus 
(TRN). All sensory messages are conveyed 
to the cortex via the thalamus (see the gure) 
( 10). The TRN is located between the thala-
mus and the cortex and, unlike other groups 
of  thalamic  neurons  (thalamic  nuclei),  is 
composed  of  inhibitory  neurons  that  are 
connected by electrical synapses (  11). These 
electrical  synapses,  together  with  inhibi-
tory chemical synapses (those that transmit 
-aminobutyric acid), can synchronize r-
ing of TRN neurons. Because TRN neurons 
project  to  other  thalamic  nuclei,  synchro-
nized activity of TRN neurons can entrain 
the activity of other thalamic regions (  10).
To measure the strength of electrical cou-
pling, Haas et al. injected depolarizing cur-
rent into one TRN neuron and measured the 
response  in  both  the  injected  cell  and  the 
noninjected  neuron. The  ratio  of  the  two 
electrical responses is dened as the cou-
pling coefcient (cc). The coupling coef-
cient among TRN neurons is large (indicat-
ing strong electrical coupling), and often a 
burst of electrical activity (action potential) 
in one neuron will produce action potential 
in the coupled neuron. The coupling coef-
ficient  can  be  estimated  in  two  ways:  by 
injecting current in cell 1 (i.e., cc
12
) or by 
injecting current in cell 2 (i.e., cc
21
). Inter-
estingly, Haas et al. found that a substantial 
number of neuron pairs exhibited asymmet-
rical  coupling. That  is,  the  distribution  of 
the ratio cc
1
/cc
2
 was skewed. In vivo, TRN 
neurons often re bursts of electrical activ-
ity (spikes). The authors found that bursts 
of spikes in pairs of coupled TRN neurons 
resulted in LTD of the strength of electri-
cal synapses. Burst activity in both neurons 
produced symmetrical LTD such that cc
12 
= 
cc
21
. However, when cell 1 was induced to 
burst while the coupled cell (cell 2) was pre-
vented from bursting (by current injection), 
the resulting LTD was asymmetrical. Under 
these conditions, the coupling measure from 
cell 1 to cell 2 (cc
12
) decreased much less than 
the coupling from the inactive cell (cc
21
) that 
was prevented from bursting. Although Hass 
et al. observed a modest decrease of synap-
tic strength, they show that LTD of electrical 
coupling is sufcient to prevent propagation 
of bursting activity among neurons.
What  are  the  mechanisms  underlying 
activity-dependent LTD of electrical syn-
apses? The  results  of  Haas  et  al.  suggest 
that  sodium-dependent  action  potentials 
may play a role (in response to a stimulus, 
sodium  channels  open  and  allow  sodium 
into  the  neuron,  which  triggers  the  fir-
NEUROSCIENCE
After burst 
activity
Inactive
Brain
Depression of electrical synapses. (Enlarged view, left side) Inhibitory neurons (circles) in the mamma-
lian thalamic reticular nucleus (TRN) are connected via electrical (small black arrows) and inhibitory chemi-
cal synapses (not illustrated). External excitatory inputs impinge on TRN neurons and can activate them. 
(Enlarged view, right side) When TRN neurons generate bursts of action potentials, electrical synapse 
strength decreases. The decrease of strength can be asymmetrical between cells that do not generate bursts 
(white arrows) and those that do (gray arrows).
C
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Department of Comparative Medicine, Stanford University, 
Stanford, CA 94305, USA. E-mail: shaul.hestrin@stanford.edu
The Strength of Electrical Synapses
Shaul Hestrin
The strength of electrical synapses in the 
mammalian brain can be modulated by 
neuronal ativity.
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  316
PERSPECTIVES
Watery Disks
PLANETARY SCIENCE
Rachel Akeson
The Herschel Space Observatory has detected 
a large reservoir of water stored as ice in the 
disk surrounding a nearby star.
ing of an action potential). In addition, an 
increase  in  cytoplasmic  calcium  concen-
tration could activate a protein kinase that 
modies (by phosphorylation) gap junction 
channels,which bridge electrically coupled 
neurons. Alternatively, partial replacement 
of nonrectifying gap junctions with rectify-
ing gap junctions (thus allowing electrical 
current to pass preferentially in one direc-
tion) is a possible mechanism.
The  functional  consequences  of  LTD 
produced by electrical synapses are of great 
interest. By producing asymmetrical changes 
of electrical coupling, the outbound connec-
tion of a group of bursting neurons will be 
stronger than the inbound connection from 
coupled neurons that did not burst. The func-
tional consequences resulting from the gen-
eration of asymmetry of electrical synapses 
within the TRN remains to be explored. The 
impact of reducing the strength of electrical 
synapses at the circuit level and their poten-
tial effect on rhythmic activity in the TRN is 
also of interest. In vivo, TRN neurons can 
switch between burst and tonic ring modes 
( 10). If these activities can induce LTD, one 
may expect to nd changes in the strength of 
electrical coupling in the TRN that correlate 
with different behavioral states during sleep 
and wakefulness. 
References
  1.  W. M. Cowan, E. R. Kandel, in Synapses, W. M. Cowan, 
T. C. Sdhof, C. F. Stevens, Eds. (Johns Hopkins Univ. 
Press, Baltimore, 2001), pp. 187.
 
2.  A. E. Pereda et al., Proc. Natl. Acad. Sci. U.S.A. 95, 
13272 (1998).  
  3.  J. S. Haas, B. Zavala, C. E. Landisman, Science 334, 389 
(2011).
  4.  S. P. Brown, S. Hestrin, Curr. Opin. Neurobiol. 14, 415 
(2009).
  5.  H. Ko et al., Nature 473, 87 (2011).  
  6.  M. Galarreta, S. Hestrin, Nature 402, 72 (1999).  
  7.  J. R. Gibson, M. Beierlein, B. W. Connors, Nature 402, 75 
(1999).  
  8.  C. E. Landisman, B. W. Connors, Science 310, 1809 
(2005).  
  9.  V. Zsiros, G. Maccaferri, J. Neurosci. 28, 1804 
(2008).  
 10.  S. M. Sherman, R. W. Guillery, in The Synaptic Orgnaiza-
tion of the Brain, G. M. Shepherd, Ed. (Oxford Univ. 
Press, Oxford, ed. 5, 2004), pp. 311359.
 11.  C. E. Landisman et al., J. Neurosci. 22, 1002 (2002). 
10.1126/science.1213894
 T
he  paradigm  for  star  formation  is 
understood to center around the for-
mation of a rotating disk from a cloud 
of gas and dust. The circumstellar disk fun-
nels material onto the newly formed central 
star and also serves as a reservoir of mate-
rial from which a planetary system may arise. 
Determining the physical and chemical com-
position of these disks is necessary to under-
stand the formation and evolution of planets. 
Previous observations have detected the pres-
ence of molecules within the disk, thereby 
demonstrating an active chemical network. 
However, this chemistry is harder to trace in 
the majority of the disk where low tempera-
tures result in the molecules freezing out onto 
grains. On page 338 of this issue, Hoger  heijde 
et al. ( 1) use the Herschel Space Observatory 
to detect cold water vapor in one of the closest 
young stars, TW Hydrae. The source of that 
water vapor is likely to be a large reservoir of 
ice grains.
In the past few decades, the basic physical 
information we have learned about circum-
stellar diskstheir mass, size, and lifetimes
come from observations of micrometer-sized 
dust grains within them. However, the vast 
majority of the material is gaseous, primarily 
molecular hydrogen. Transitions of molecular 
hydrogen are very difcult to observe, and the 
only H
2
 detections in disks are of warm gas 
in the center. Attention has therefore turned to 
other molecules such as CO, HCO
+
, and CN 
to trace the gaseous component.
Water  is  the  main  constituent  of  the 
mantles on grains found in the low-density 
medium  that  fills  the  space  between  stars 
and can serve as an oxygen reservoir in the 
gas  phase. Thus,  water  may  be  one  of  the 
key components in the chemistry and ther-
mal  balance  of  both  the  parent  cloud  and 
the circumstellar disk. Spectroscopic obser-
vations  of  water  vapor  from  ground-based 
telescopes are hindered by water vapor fea-
tures in Earths atmosphere. In the inner disk, 
where water is present as hot vapor and can 
be observed from the ground, observations 
have shown water vapor at abundances above 
the levels measured in molecular clouds (  2). 
These  observations  include  the  so-called 
habitable zone where terrestrial planets are 
believed to have formed in our solar system. 
However, most of the mass within the disk is 
NASA Exoplanet Science Institute, California Institute of 
Technology, Pasadena, CA 91125, USA. E-mail: rla@ipac.
caltech.edu
Rocky planetesimals Icy planetesimals
Snow line
 A frozen line of division. Interior to the snow line, planetesimals forming in the disk are rocky, while out-
side they are icy. In our solar system, this line corresponds to the divide between the inner terrestrial planets 
and the outer gas giants. C
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www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   317
PERSPECTIVES
below the 150 K condensation temperature 
for water, and thus most water exists as ice 
on grains. Spectroscopic features from water 
ice have been seen (  3,  4), but these techniques 
have only been applied to a few objects with 
favorable viewing geometries. Observations 
of the water isotope HDO (D is deuterium) 
in the gas phase of the outer disk led to mod-
els  of  ultraviolet  photons  from  the  central 
star desorbing water molecules from the icy 
grains back into the gas phase (  5). The obser-
vations of Hogerheijde et al. are consistent 
with this cycle. Their calculations show that 
a large population of icy grains, equivalent to 
several thousand Earth oceans, is necessary 
to maintain the observed level of water vapor 
on the surface of the disk.
Water can also play a critical role in the 
formation and nal surface composition of 
planets.  Ice  enhances  the  solid  material  in 
the cold outer part of a protoplanetary disk, 
which  promotes  the  formation  of  cores  of 
gaseous planets (  6). The disk radius where 
ice can condense is often termed the snow 
line, and the location of this line is a property 
of the stellar mass and disk evolutionary state 
(see the gure). The location and evolution of 
this snow line may affect the formation rate of 
large planets ( 7).
The distribution of water ice in the cir-
cumstellar  disk  can  also  help  address  the 
issue  of  where  Earths  water  originated. 
While  forming,  Earth  is  believed  to  have 
been too hot to have liquid water and would 
have retained little water vapor from the gas-
eous component of the disk. Thus, the water 
we have now arrived later, most likely from 
ice-covered  comets  or  asteroids  from  the 
outer parts of the solar system. In addition 
to the water abundance, the spectra obtained 
by Hogerheijde et al. allow determination of 
the spin isomer ratio, where the spin refers 
to the alignment of the hydrogen proton spin 
vectors (that is, the ratio of the amount of 
para- to ortho-hydrogen in the water mole-
cules). They found a ratio much lower than 
that measured for solar system comets, sug-
gesting that material from multiple locations 
in the TW Hydrae disk is mixed before incor-
poration  into  larger  bodies.  Evidence  for 
such radial transport in the early solar sys-
tem includes results from the Stardust mis-
sion that returned comet samples containing 
material formed at high temperatures ( 8).
As  the  number  of  planets  discovered 
around other stars expands to include many 
systems with multiple planets, it is clear that 
the  universe  includes  many  planetary  sys-
tem architectures very different from that of 
our own solar system. To constrain models 
of  planet  formation,  including  the  chemi-
cal composition, we need to understand the 
distribution  and  evolution  of  molecules  in 
the disk, including water, a key catalyst for 
life on Earth. The next several years will pro-
vide many opportunities to progress in this 
study  as  Herschel  and  other  observatories 
will  make  spectroscopic  observations  of  a 
much larger sample of disks covering a range 
of stellar age and mass. Also, new facilities, 
such as the Atacama Large Millimeter Array, 
will greatly expand on the current sensitivity 
levels to allow spatially resolved observations 
of molecules in the disk. 
References
  1.  M. R. Hogerheijde et al., Science 334, 338 (2011).
  2.  J. S. Carr, J. R. Najita, Science 319, 1504 (2008).  
  3.  K. M. Pontoppidan et al., Astrophys. J. 622, 463 (2005).  
  4.  M. Honda et al., Astrophys. J. 690, L110 (2009).  
  5.  C. Ceccarelli, C. Dominik, E. Caux, B. Leoch, P. Caselli, 
Astrophys. J. 631, L81 (2005).  
  6.  C. Hayashi, K. Nakazawa, Y. Nakagawa, Protostars and 
Planets II (University of Arizona Press, Tucson, 2005), 
pp. 11001153.
  7.  G. M. Kennedy, S. J. Kenyon, Astrophys. J. 673, 502 
(2008).  
  8.  T. Nakamura et al., Science 321, 1664 (2008).  
10.1126/science.1213752
Antenna-Guided Light
APPLIED PHYSICS
Nader Engheta
Compact arrays of gold nanoantennas can 
be used to create optical structures that bend 
the path of light in unusual ways.
 T
he bent appearance of a stick half-sub-
merged in water is caused by the dif-
ference in refractive indices of air and 
waterlight travels more slowly in water than 
in air (see the gure, panel A) and refracts and 
reects off the air-water interface. Snells law 
(  1) lets us calculate the bending angle if we 
know the geometry and the refractive indices. 
In complex optical instruments, where sev-
eral lenses, mirrors, and other components 
may be present, designers control the bending 
by keeping track of the phase shifts imposed 
along the wavefront of the light; for exam-
ple, a light beam can be focused by different 
phase shifts that occur along a curved lens. 
These optical components are much larger 
than the wavelength of light, which limits the 
minimum size of devices. On page 333 of this 
issue, Yu et al. ( 2) show how arrays of struc-
tures smaller than the wavelength of light, 
V-shaped nanoantennas made of gold, bend 
light by creating abrupt phase shifts through 
the  excitation  of  resonances. The  authors 
show that these compact metasurfaces fol-
low a more general version of Snells law that 
accounts for the bending of a light beam in 
unconventional but potentially useful ways.
Conventionally, the bending of light may 
occur at an abrupt interface of two media 
(e.g., air and water), or through a gradual 
change of refractive index (e.g., air above 
the hot desert roads causes mirage; see the 
figure,  panel  B).  However,  it  is  possible 
to obtain the desired phase shift along the 
wavefront  by  tailoring  planar  interfaces. 
One  of  the  early  examples  is  the  Fresnel 
lens, in which a set of concentric lenses are 
cut to different curvatures and impose dif-
ferent phase shifts. Although a Fresnel lens 
is much thinner than an equivalent conven-
tional lens, its thickness is still far greater 
than the wavelength of light.
Light  does  not  always  simply  pass 
through a medium; it can also excite reso-
nances that can lead to absorption and emis-
sion. For the much longer wavelengths of 
light used in radio and microwave com-
munications, antennas called reectarrays 
( 3) and transmitarrays ( 4) contain multiple 
antenna elements that act as resonators to 
control  the  direction  in  which  signals  are 
received  or  broadcast.  However,  the  reso-
nant elements responsible for the required 
phase shift and their arrangement in peri-
odic arrays are still comparable in size to 
the  wavelength  of  operation  (  3  5). These 
devices  often  operate  over  only  a  narrow 
range of frequencies.
For  shorter-wavelength  light,  such  as 
infrared and visible light, plasmonic phenom-
enathe excitation of collective oscillations 
of  electrons  in  materials  such  as  gold  and 
silvercan allow subwavelength objects to 
undergo resonance responses in the scatter-
ing process. Yu et al. designed subwavelength 
University of Pennsylvania, Department of Electrical and 
Systems Engineering, Philadelphia, PA 19104, USA. E-mail: 
engheta@ee.upenn.edu
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  318
PERSPECTIVES
gold antennas with a V shape; they varied the 
scattering of light by changing the length of 
the arm and the angle and the orientation of 
these Vs. The phase difference between the 
scattered and incident elds is tailored over a 
small distance along the lights path, that is, 
the structures are optically thin.
Yu  et  al.  printed  planar  arrays  of  such 
V-shaped nanoantennas in suitably designed 
patterns on a silicon wafer and demonstrated 
several intriguing light-bending scenarios at 
these metasurfaces, including unconventional 
reection and refraction angles, total internal 
reflections  with  two  critical  angles  (rather 
than only one), and reected light becoming 
evanescent (diminishing in amplitude with 
distance away from the interface, rather than 
propagating) at certain angles. None of these 
effects are predicted from the conventional 
Snells law, but they do follow a generalized 
version derived by the authors that allows for 
desired variations of the change of phase on 
the interface.
These  arrays  of  nanoantennas,  which 
could  include  movable  sections,  could  be 
used to design photonic components such as 
lenses and mirrors that are ultrathin, confor-
mal (angle-preserving), and even deform-
able.  Reconfigurable  couplers  and  wave-
guides, which could be driven by electric, 
magnetic, or optical stimuli, may be envi-
sioned that could guide and mix light beams 
through almost arbitrary paths chosen along 
a surface. Yu et al. have also created optical 
vortices with orbital angular momentum ( 6) 
by impinging a beam at normal incidence on 
the specially designed planar metasurface of 
these V-shaped nanoantennas. Such vortices 
could nd use in applications such as opti-
cal tweezers.
Metasurfaces (  7) are the planar version 
of metamaterials that are engineered to con-
trol and tailor the light interaction in uncon-
ventional ways (for example, creating mate-
rials with optical band gaps that completely 
reect light over a given frequency range). 
In  the  three-dimensional  metamaterials,  it 
can be difcult to engineer a structure that 
maintains  its  designed  performance  and 
avoids performing like a bulk material. Meta-
surfaces may offer advantages in this regard 
because their constituent resonant elements 
are  all  distributed  in  a  planar  surface  and 
more readily assembled. This type of two-
dimensional structure will add another tool 
to the eld of transformation optics (  8,  9), in 
which a prescribed change (such as a phase 
shift or amplitude variation) is designed into 
the light path for applications such as cloak-
ing, or where metasurfaces are used to creat-
ing highly conned cavity modes ( 10,   11) of 
potential interest in quantum optics. 
References
  1.  M. Born, E. Wolf, Principles of Optics (Pergamon, 
Oxford, 1980).
  2.  N. Yu et al., Science 334, 333 (2011).  
  3.  D. M. Pozar, S. D. Targonski, H. D. Syrigos, IEEE Trans. 
Antenn. Propag. 45, 287 (1997).  
  4.  C. G. M. Ryan et al., IEEE Trans. Antenn. Propag. 58, 
1486 (2010).  
  5.  N. Bliznyuk, N. Engheta, Mic. Opt. Tech. Lett. 40, 361 
(2004).  
  6.  M. Padgett, J. Courtial, L. Allen, Phys. Today 57, 35 
(2004).  
  7.  E. F. Kuester, M. A. Mohamed, M. Piket-May, C. L. Hol-
loway, IEEE Trans. Antenn. Propag. 51, 2641 (2003).  
  8.  J. B. Pendry, D. Schurig, D. R. Smith, Science 312, 1780 
(2006).  
  9.  U. Leonhardt, Science 312, 1777 (2006).  
 10.  M. Caiazzo, S. Maci,, N. Engheta, IEEE Antenn. Wirel. 
Propag. Lett. 3, 261 (2004).  
 11.  C. L. Holloway, D. C. Love, E. F. Kuester, A. Salandrino, N. 
Engheta, IET Microwave Antenn. Propag. 2, 120 (2008).  
A
C   D B
L >>  L >> 
d  
5 m
Bending light, big and small. Several mechanisms for bending light are depicted. The optical structures 
shown in (A) and (B) are much larger than the wavelength of light. In (A), an interface between two media 
with two different indices of refraction bends light. In (B), light is bent by a material that gradually changes 
refractive index with distance. Yu et al. caused the bending of light in unusual ways (C) with thin metasur-
faces. These metasurfaces contain distributed arrays of gold nanoantennas (D) that are smaller than the 
wavelength of light. In such arrays, the proper patterns of phase changes created by resonant nanostructures 
lead to bending effects not anticipated by conventional laws of reection and refraction in optics.
10.1126/science.1213278
 T
he  advent  of  satellite-based  remote 
sensing  of  ocean  color  in  the  late 
1970s  (  1)  provided  the  first  large-
scale views of chlorophyll distributions in 
the  upper  ocean.  These  distributions  are 
a proxy for the biomass of phytoplankton, 
which  drive  oceanic  productivity.  More 
recently,  ocean  color  measurements  have 
been combined with satellite data on sea-
surface  height  (SSH)  and  other  physical 
properties of the ocean to elucidate the pro-
cesses that regulate primary production in 
the sea. On page 328 of this issue, Chelton et 
al. ( 2) further advance this eld by showing 
that ocean eddies exert a strong inuence on 
near-surface chlorophyll.
Initial  comparisons  (  3,   4)  of  satellite 
ocean  color  measurements  and  SSH  data 
showed that some of the variability in ocean 
color was associated with large-scale SSH 
patterns that propagate westward in extra-
tropical  latitudes.  The  authors  attributed 
these patterns to planetary or Rossby waves, 
which are freely propagating modes of large-
scale  variability  in  the  ocean.  Four  basic 
processes  have  been  proposed  to  explain 
the  observed  relations,  including  lateral 
Eddies Masquerade as 
Planetary Waves
OCEANS
Dennis J. McGillicuddy Jr.
Variabilities in sea-level and upper-ocean chlorophyll reveal the systematic inuence of 
nonlinear eddies.
Woods Hole Oceanographic Institution, Woods Hole, MA 
025431541, USA. E-mail: dmcgillicuddy@whoi.edu
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   319
PERSPECTIVES
advection  of  the  mean  chlorophyll  gradi-
ent, uplift of the deep chlorophyll maximum 
into the surface layer, enhancement of phy-
toplankton biomass stimulated by upwelling 
of nutrients, and accumulation of material 
in convergence zones within the planetary 
wave eld ( 5 7).
These  early  studies  focused  on  large-
scale signals characteristic of Rossby waves 
by  processing  the  satellite  measurements 
with scale-selective lters. This processing 
was intended to remove seasonal variability 
as well as the effects of mesoscale (tens to 
hundreds of kilometers) eddiesubiquitous 
features  of  ocean  circulation  (sometimes 
referred to as the internal weather of the sea) 
that result from both direct forcing and inter-
nal instability processes.
Merging data from multiple satellite mis-
sions led to altimetric data sets ( 8  10) with 
higher resolution than used previously, but 
it remains difcult to differentiate between 
Rossby waves and eddies in the merged data 
sets. Single Rossby waves (see the gure, 
panel A) are rarely if ever observed in the 
ocean, but superposition of multiple Rossby 
waves can result in eddy-like features (panel 
A, inset) that are similar to the patterns seen 
in altimeter data (panel B). However, plane-
tary waves and eddies have different degrees 
of nonlinearity: Nonlinear eddies trap uid 
inside them, whereas linearly propagating 
wavelike  disturbances  do  not. The  degree 
of nonlinearity can be estimated as the ratio 
between  an  eddys  swirl  velocity  and  its 
translation speed.
Previously, Chelton and co-workers used 
this insight to show that mid-latitude SSH 
variability is dominated by westward-prop-
agating  nonlinear  eddies,  and  developed 
automated tracking algorithms to compile a 
global synthesis of eddy trajectories ( 9,  10). 
Chelton et al. have now overlaid those eddy 
tracks on the westward-propagating signals 
previously  attributed  to  Rossby  waves  in 
the ltered SSH and ocean color data. The 
results strongly suggest that eddies are driv-
ing these signals ( 2).
How might mesoscale eddies masquer-
ade as larger-scale Rossby waves? Due to 
the latitudinal dependence of the effects of 
Earths rotation, both types of features move 
westward at roughly the same speed. More-
over,  Chelton  et  al.  show  that  the  statisti-
cal properties of a patchwork of westward-
propagating eddies are qualitatively similar 
to  those  expected  for  Rossby  waves. This 
observation explains why eddies can pass 
through  the  filters  intended  to  eliminate 
them in earlier studies.
Chelton et al.s ndings require reassess-
ment of the underlying mechanisms used to 
explain satellite observations of variability in 
SSH and upper-ocean chlorophyll. Although 
the  same  four  basic  processes  of  biomass 
modulation  mentioned  above  for  Rossby 
waves remain valid for eddies, lateral advec-
tion of the mean chlorophyll gradient is the 
dominant mechanism revealed in Chelton et 
al.s analysis. However, the relative impor-
tance of each of the four processes can vary 
with oceanographic regime and scale, rang-
ing from the mesoscale down to the submeso-
scale ( 11  13). At present, submesoscale fea-
tures are not resolved by operational remote-
sensing technology for SSH.
Although  higher-resolution  data  are 
expected  in  the  future  for  both  SSH  and 
ocean color, in situ observations will con-
tinue to be critical for those variables that 
cannot be measured from space. Moreover, 
because near-surface waters are depleted in 
nutrients  over  large  areas  of  the  mid-lati-
tudes, key aspects of the biological response 
to physical perturbations take place too deep 
to be detected by satellite ocean color imag-
ery (  14). Although Chelton et al.s results 
must be interpreted with that caveat, their 
ndings constitute a key step forward in our 
understanding of physical-biological inter-
actions in the ocean, with important rami-
cations for both ecosystem dynamics and 
biogeochemical cycling. 
References and Notes
  1.  J. F. R. Gower, K. L. Denman, R. J. Holyer, Nature 288, 
157 (1980).  
  2.  D. B. Chelton, P. Gaube, M. G. Schlax, J. J. Early, R. M. 
Samelson, Science 334, 328 (2011); 10.1126/
science.1208897.  
  3.  B. M. Uz, J. A. Yoder, V. Osychny, Nature 409, 597 
(2001).  
  4.  P. Cipollini, D. Cromwell, P. G. Challenor, S. Raffaglio, 
Geophys. Res. Lett. 28, 323 (2001).  
  5.  P. D. Killworth, P. Cipollini, B. M. Uz, J. R. Blundell,
 J. Geophys. Res. 109, C07002 (2004).  
  6.  Y. Dandonneau, A. Vega, H. Loisel, Y. du Penhoat, 
C. Menkes, Science 302, 1548 (2003).  
  7.  G. Charria, F. Mlin, I. Dadou, M.-H. Radenac, V. Garon, 
Geophys. Res. Lett. 30, 1125 (2003).  
  8.  A. Pascual, Y. Faugre, G. Larnicol, P.-Y. Le Traon, 
Geophys. Res. Lett. 33, L02611 (2006).  
  9.  D. B. Chelton, M. G. Schlax, R. M. Samelson, Prog. 
Oceanogr. 91, 167 (2011).  
 10.  D. B. Chelton, M. G. Schlax, R. M. Samelson, R. A. de 
Szoeke, Geophys. Res. Lett. 34, L15606 (2007).  
 11.  M. Lvy, P. Klein, A.-M. Treguier, J. Mar. Res. 59, 535 
(2001).  
 12.  E. R. Abraham, Nature 391, 577 (1998).  
 13.  D. A. Siegel, P. Peterson, D. J. McGillicuddy Jr., S. Mari-
torena, N. B. Nelson, Geophys. Res. Lett. 38, L13608 
(2011).  
 14.  D. J. McGillicuddy Jr. et al., Science 316, 1021 (2007).  
 15.  J. C. McWilliams, G. R. Flierl, Deep-Sea Res. 23, 285 
(1976).
 16.  Altimeter data were produced and distributed by AVISO 
(www.aviso.oceanobs.com) as part of the SSALTO ground-
processing segment.
 17.  I thank NSF and NASA for support and L. Anderson for 
preparing the gure.
Rossby waves Satellite altimeter
Single wave
Superposition of 4 waves
Longitude  (W)
L
a
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A
70 65 60 55 70 65 60 55
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Longitude (W)
 
S
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a
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e
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e
l
 
a
n
o
m
a
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(
c
m
)
B
29
32
35
20
10
0
10
20
Rossby waves and eddies. (A) A model of a single Rossby wave propagating 
through a still ocean leads to a highly regular sea-level anomaly pattern. If sev-
eral such waves are superposed, an eddy-like pattern results (inset) ( 15). (B) 
Mapped observations ( 16) of sea-level anomaly for a region of the western North 
Atlantic on 17 June 2005. Satellite ground tracks are shown as dotted lines. 
Although the patterns seen in the altimeter data resemble those of the super-
posed Rossby waves, Chelton et al. show that they are in fact caused by nonlinear 
mesoscale eddies.
10.1126/science.1208892
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  320
PERSPECTIVES
 C
ells, and the organelles within them, 
are  surrounded  by  lipid-bilayer 
membranes  that  compartmentalize 
biochemical reactions and pathways. Mem-
brane-embedded  proteins  control  the  ux 
of molecules, energy, and information such 
that  the  segregated  compartments  func-
tion  as  a  unied  living  cell. Traditionally, 
membrane proteins were pictured as oat-
ing around quite independently of the sur-
rounding lipids, yet when this uid-mosaic 
model was described, Singer and Nicolson 
qualied that a small fraction of the lipid 
may interact specically with the membrane 
proteins (  1). It has taken 40 years to fully 
appreciate the importance of this assertion. 
On page 380 of this issue, Zhou et al. ( 2) 
report mass spectrometry of intact integral 
membrane  protein  complexes  solubilized 
from bilayers. The results show that specic 
structural  lipids  remain  bound  in  the  gas 
phase and can be counted.
Despite some technical hurdles, integral 
membrane  proteins  and  their  complexes 
have proven amenable to the soft ionization 
technologies of biological mass spectrom-
etry. Intact complexes are isolated by gen-
tle solubilization of membranes with mild 
nonionic detergent, followed by biochemi-
cal isolation within a detergent micelle for 
solubility. Earlier studies next used organic 
solvents to break noncovalent associations 
with lipids and between subunits. Chroma-
tography in aqueous/organic mixtures cou-
pled to mass spectrometry provided intact 
molecular mass proles of individual sub-
units  and  their  covalent  modifications  on 
low-resolution analyzers ( 3,   4). Top-down 
dissociation experiments on high-resolution 
Fourier-transform instruments yielded fully 
assigned primary structures with high statis-
tical condence (  5,   6).
However, if the complexes could be ana-
lyzed intact, subunit stoichiometry and the 
presence of intimate cofactors such as spe-
cific  lipid  molecules  could  also  be  deter-
mined. In 2004, Robinsons group realized 
that electrospray ionization could be used 
to transfer membrane-protein micelles from 
aqueous solutions into the gas phase, with 
subsequent depletion of detergent in vacuo 
( 7). Development of this native mass spec-
trometry approach has enabled the measure-
ment of bound lipid stoichiometry in mem-
brane lipid-protein complexes described by 
Zhou et al.
The  detection  of  lipids  within  integral 
membrane protein structures requires care-
ful  solubilization  to  preserve  native  asso-
ciations. This is important because micelle-
forming detergents tend to displace lipids, 
even while preserving protein subunit inter-
actions. For example, successful crystalliza-
tion of the cytochrome b
6
f complex required 
addition of lipids to isolated complexes, even 
though  preparations  retained  some  native 
lipids ( 8,  9).
As early as 1973, Santiago et al. argued, 
based  upon  lipid-peroxidation/protection 
data, for the specic requirement of the lipid 
cardiolipin for rat mitochondrial adenosine 
triphosphatase  (ATPase)  activity  (see  the 
gure, left), concluding that specic lipids 
were critical to the function of this integral 
membrane protein complex ( 10). Apprecia-
tion of the importance of specically bound 
lipids to the structure and function of inte-
gral membrane proteins has grown steadily 
as x-ray crystallography has provided ever 
more  examples  from  numerous  membrane 
proteins. Cardiolipin was rst resolved in the 
structure of the purple bacterial reaction cen-
ter (  11) and later shown to provide thermal 
stability to the structure (  12). Although the 
structure of bovine mitochondrial rotary ATP 
synthase has been solved, cardiolipin was not 
seen, presumably due to its displacement by 
detergent ( 13).
The  rotary  ATP  synthases  couple  the 
electrochemical energy of a transmembrane 
proton gradient to synthesis of ATP; proton 
movement  through  an  integral  membrane 
ring of subunits causes rotation of this rotor 
relative  to  a  stationary  integral  stator  and 
associated extrinsic subunits, driving confor-
mational changes that facilitate ATP synthe-
sis ( 14). The number of rotor subunits varies 
across living organisms, with those having 
the least subunits synthesizing the most ATP 
per  proton  translocated.  Current  research 
explores the role of bound lipids in the rotor 
structure, and measurements of the number 
of  bound  lipids  and  their  binding  sites  by 
mass spectrometry should thus help resolve 
some of the outstanding details of the mecha-
nism of rotary coupling.
Zhou et al. use native electrospray-ion-
ization mass spectrometry to measure rotor 
subunit  and  bound  lipid  stoichiometry  in 
two intact rotary ATPases from the bacteria 
Thermus  thermophilus  and  Enterococcus 
hirae. The results show that the solubilized 
T. thermophilus complex has a ring with 12 
subunits, with 6 phosphatidylethanolamine 
lipids bound to it, whereas the E. hirae rotor 
has  10  subunits  with  10  cardiolipins. The 
Up Close with Membrane 
Lipid-Protein Complexes
STRUCTURAL BIOLOGY
Julian Whitelegge
State-of-the-art mass spectrometry reveals 
how many specic lipids are bound to 
membrane proteins.
O
O
P O
O
O
O
OH
O
O
O
O
P
O
O
O
O
O
O
Cardiolipin
Along for the ride. Cardiolipin (left) is an 
unusual phospholipid with four fatty acyl 
chains. In the integral membrane rotor of 
the eight-membered vertebrate mitochon-
drial ATP synthase (right), each of four 
cardiolipin molecules binds the four trans-
membrane domains of two ring subunits.
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NPI-Semel Institute for Neuroscience and Human Behav-
ior, University of California at Los Angeles, Los Angeles, CA 
900241759, USA. E-mail: jpw@chem.ucla.edu
www.sciencemag.org    SCIENCE    VOL 334    21 OCTOBER 2011   321
PERSPECTIVES
Every Bit Counts
CELL SIGNALING
Peter J. Thomas
Information theory is applied to cell biology 
to determine the processing properties of 
signaling pathways and the consequences 
of noise.
authors picture the T. thermophilus complex 
as six dimers each with a single lipid, con-
sistent with electron microscopy images that 
support a hexameric structure (  15). The E. 
hirae complex has 10 monomers, each with a 
bound cardiolipin, correcting a crystal struc-
ture with misassigned lipids (  16).
These measurements cover a range of 0.5 
to 2 lipid fatty acyl chains per transmembrane 
domain within the rotor, consistent with the 
value of one inferred from the measurement 
of four cardiolipin per eight-subunit verte-
brate mitochondrial ATPase rotor using 
31
P 
nuclear magnetic resonance (NMR) (  17). The 
16 transmembrane domains that, along with 
four intimately associated cardiolipins, make 
up this eight-membered ring (see the gure, 
right) function as the smallest natural ATPase 
rotor, accounting for the maximal efciency 
of ATP  synthase  activity  observed  for  this 
complex (13).
Zhou et al. go on to show that gas-phase 
dissociation patterns are sensitive to pH and 
the presence of nucleotides, suggesting con-
formational changes within the complexes. 
This  conclusion  is  further  supported  by 
gas-phase ion mobility mass spectrometry 
experiments that elegantly demonstrate the 
technological sophistication of the instru-
mentation used (  2). The authors further dis-
cuss  how  rearrangement  of  lipid-protein 
interactions might serve to modulate ATP 
synthase/ATPase activities.
The  ability  to  profile  intact  membrane 
lipid-protein complexes and detect organiza-
tional changes related to dynamic processes 
by mass spectrometry, as reported by Zhou 
et  al.,  will  empower  our  understanding  of 
the functioning of biological membranes. A 
new class of neopentyl glycol detergents that 
appear to solubilize membrane lipid-protein 
complexes  with  minimal  structural  pertur-
bation bodes well for native mass spectrom-
etry ( 18). Future research should also aim to 
elucidate the role of bilayers in general, as 
well as the specic lipid-protein associations 
discussed  above,  in  the  insertion,  folding, 
assembly, function, and regulation of integral 
membrane proteins. 
References
  1.  S. J. Singer, G. L. Nicolson, Science 175, 720 (1972).  
  2.  M. Zhou et al., Science 334, 380 (2011).
  3.  I. M. Fearnley, J. E. Walker, Biochem. Soc. Trans. 24, 912 
(1996). 
  4.  J. P. Whitelegge, H. Zhang, R. Aguilera, R. M. Taylor, 
W. A. Cramer, Mol. Cell. Proteomics 1, 816 (2002).  
  5.  B. Thangaraj et al., Proteomics 10, 3644 (2010).  
  6.  C. M. Ryan et al., Mol. Cell. Proteomics 9, 791 (2010).  
  7.  L. L. Ilag, I. Ubarretxena-Belandia, C. G. Tate, C. V. 
Robinson, J. Am. Chem. Soc. 126, 14362 (2004).  
  8.  H. Zhang, G. Kurisu, J. L. Smith, W. A. Cramer, Proc. 
Natl. Acad. Sci. U.S.A. 100, 5160 (2003).  
  9.  S. S. Hasan et al., J. Mol. Biol. (2011), 10.1016/
j.jmb.2011.09.023.
 10.  E. Santiago, N. Lpez-Moratalla, J. F. Segovia, Biochem. 
Biophys. Res. Commun. 53, 439 (1973).  
 11.  K. E. McAuley et al., Proc. Natl. Acad. Sci. U.S.A. 96, 
14706 (1999).  
 12.  P. K. Fyfe, N. W. Isaacs, R. J. Cogdell, M. R. Jones, 
Biochim. Biophys. Acta 1608, 11 (2004).  
 13.  I. N. Watt, M. G. Montgomery, M. J. Runswick, A. G. 
Leslie, J. E. Walker, Proc. Natl. Acad. Sci. U.S.A. 107, 
16823 (2010).  
 14.  D. Stock, A. G. Leslie, J. E. Walker, Science 286, 1700 
(1999).  
 15.  R. A. Bernal, D. Stock, Structure 12, 1789 (2004).  
 16.  T. Murata, I. Yamato, Y. Kakinuma, A. G. Leslie, J. E. 
Walker, Science 308, 654 (2005).  
 17.  K. S. Eble, W. B. Coleman, R. R. Hantgan, C. C. 
Cunningham, J. Biol. Chem. 265, 19434 (1990). 
 18.  P. S. Chae et al., Nat. Meth. 7, 1003 (2010).  
10.1126/science.1214084
 T
he term signal transduction has been 
in use for over 40 years, originating in 
biological  studies  of  cellular  photo-
receptors  and  chemotaxis,  and  elaborated 
through  discoveries  of  signaling  systems 
such as the protein kinases ( 1). In engineer-
ing, signaling has a precise meaning that 
denes the notion of information (  2), and 
quanties the capabilities of a signaling sys-
tem in terms of its channel capacity, measured 
in bits ( 3). Despite the attractive analogy, a 
number of obstacles have thwarted attempts 
to  apply  information  theory  quantitatively 
to cellular signal transduction networks. On 
page 354 of this issue, Cheong et al. ( 4) suc-
ceed in doing so, making rigorous and quan-
titative measurements of information capaci-
ties in a biochemical signaling system.
A rigorous analysis of signaling requires 
a  well-defined  communications  channel, 
including an ensemble of channel inputs as 
well as outputs that are conditional on each 
possible input (see the gure). In a biological 
setting, it is not always clear what denes the 
appropriate ensembles. Cheong et al. use the 
signaling pathway engaged by tumor necro-
sis factor (TNF), which stimulates a host of 
intracellular responses mediated by two tran-
scription factors, nuclear factor kappa B (NF-
B)  and  activating  transcription  factor2 
(ATF-2). The TNF concentration serves as 
the input to the channel, and the NF-B and 
ATF-2 responses serve as outputs.
Estimating  channel  capacities  requires 
estimating the entropy of probability distri-
butions, which is a notoriously data-inten-
sive  undertaking.  Channel  capacities  and 
quantities such as information per spike 
have  been  estimated  for  neural  networks 
in systems with large ring (activity) rates 
( 5). Previous attempts to accomplish a sim-
ilar analysis in a biochemical signaling sys-
tem have not been convincing. Using quan-
titative  immunocytochemistry,  Cheong  et 
al. obtained four-dimensional arrays of data 
(time, dosage, genotype, and pathway) for 
thousands  of  individually  resolved  cells. 
With this much data, it becomes possible to 
estimate the entropies required to establish 
the channel capacity, accounting for known 
biases in entropy measurements due to nite 
(but large) sample sizes.
Biochemical  systems  often  form  net-
works  with  multiple  interactions  (cross 
talk)  that  make  the  analysis  of  statistical 
dependencies,  and  hence  channel  capaci-
ties, problematic. Here, Cheong et al. mea-
sured two readouts in the same system. The 
amount of information carried by the com-
bination of the ATF-2 and the NF-B path-
way depends, in principle, on the topology 
of interactions between the pathways. If both 
pathways get their information directly from 
the  incoming  signal,  the  mutual  informa-
tion of the two responses taken together can 
potentially be substantially increased. This 
situation is described as a bush topology, 
because the signals propagate directly along 
multiple branches from the root of the net-
work. Alternatively, the network could have 
a tree topology, in which the input signal 
passes through a common intermediate (the 
trunk of the tree) before going to independent 
readout  branches.  Remarkably,  the  differ-
Departments  of  Mathematics,  Biology,  and  Cognitive 
Science, Case Western Reserve University, Cleveland, OH 
44106, USA. E-mail: pjthomas@case.edu
21 OCTOBER 2011    VOL 334    SCIENCE    www.sciencemag.org  322
PERSPECTIVES
ence in the mutual information predicted in 
these two scenarios is large enough, and the 
data set collected by the authors substantial 
enough, to unambiguously identify the TNF
NF-BATF-2 network as having a treelike, 
rather than bushlike, topology. Each pathway 
alone carries just short of one bit of informa-
tion. [In information theory, one bit, or one 
binary digit, is the information needed to dis-
tinguish exactly two equally likely outcomes 
of an experiment (e.g., heads versus tails in a 
fair coin toss). Two bits is enough informa-
tion to distinguish four outcomes, and N bits 
is enough information to distinguish 2
N
 out-
comes.] However, the joint response of both 
pathways carries just over one bit, enough to 
reliably distinguish a single yes-no decision, 
such as presence or absence of TNF. Indeed, 
the treelike topology likely reects the fact 
that before branching out to stimulate multi-
ple pathways, the TNF response is mediated 
by a single receptor signaling (and pathway 
activation) complex. As the authors show, this 
arrangement limits the capacity of the net-
work. Even if an unlimited number of inde-
pendent pathways separately read the output 
of the TNF receptor complex, the information 
obtained by a single cell about the amount of 
stimulatory TNF cannot exceed about 1.25 
bits, which is only slightly more than from the 
NF-B and ATF-2 pathways alone.
The capacity of any channel is intimately 
related to the nature of the noise affecting the 
input-output relationship, and it can be dif-
cult to establish quantitative characteristics 
of the noise sources present in a biochemical 
channel. In engineering, one usually consid-
ers the properties of a communications chan-
nel  (such  as  a  telegraph  line  or  ber  optic 
cable)  as  fixed,  and  the  engineering  prob-
lem amounts to choosing the best encoding 
scheme given the (noisy) signal transmission 
equipment. A decade ago, it was proposed 
that biological information channels should 
be sculpted by evolutionary pressures so as 
to match to the information sources that feed 
into  them  (  6).  In  sensory  neural  systems, 
source-channel matching takes the form of 
redundancy  reduction  and  efcient  coding 
( 7 9). The pioneering work by Cheong et al. 
opens the door to similar analyses for bio-
chemical signaling systems.
The  biggest  surprise  in  the  analysis  of 
Cheong  et  al.  is  how  small  the  informa-
tion capacity of the TNF signaling system 
appears  to  be.  Noise  suppression  in  bio-
chemical  systems  is  notoriously  challeng-
ing for cells to implement (and for investi-
gators to analyze) (  10). Possible strategies 
for increasing the information about a signal 
such as TNF concentration include reduc-
ing noise by introducing a negative-feedback 
loop,  averaging  over  noise  by  integrating 
received signals over time, or pooling infor-
mation  across  multiple  cells. The  authors 
explore each possibility. Negative feedback 
proves to be a double-edged sword: It can 
reduce the amount of noise in transducing a 
signal, which tends to boost capacity, but it 
can also restrict the dynamic range of the sig-
nal input, reducing capacity. In a mutant cell 
line lacking a certain negative-feedback loop 
that normally inhibits the TNF receptor com-
plex, the authors found increased informa-
tion capacity in the short term (output at 30 
min after stimulation) but decreased capac-
ity in the long term (4 hours after stimula-
tion). In both cases, however, the information 
capacity  was  still  approximately 
one  bit.  [In  a  signaling  system 
comprising a rate-modulated Pois-
son  processfor  example,  com-
municating  by  directly  detecting 
occurrence of chemical events
it  can  be  proven  mathematically 
that feedback cannot increase the 
channel capacity ( 11).] Integration 
over time (or averaging over time) 
does not fare much better, because 
once  activated,  NF-B  activity 
remains approximately constant in 
any given cell. In other biochemi-
cal systems, time integration could 
still play a role in noise reduction. 
Of the strategies explored, pooling 
information across multiple cells 
that  each  independently  process 
the same input signal (an example 
of  the  bush  topology)  holds  the 
most promise. The authors show 
that readouts from local pools of 14 cells give 
twice the information of single cells alone.
We can look forward to more contribu-
tions from information theory to cell biol-
ogy  (and  vice  versa),  particularly  in  gra-
dient sensing the process by which motile 
eukaryotic  cells  orient  themselves  during 
chemotaxis ( 12). In this process, the ensem-
ble of inputs is all the possible directions of 
the chemoattractant gradient ( 13 15).
In 2002, Berger asserted that biology had 
become  positioned  to  prot  meaningfully 
from an invasion by information theorists 
( 6).  Nearly  a  decade  later,  the  invasion  is 
well under way and shows no sign of slow-
ing down. 
References
  1.  T. Hunter, B. M. Sefton, Proc. Natl. Acad. Sci. U.S.A. 77, 
1311 (1980).  
  2.  C. Shannon, Bell Syst. Tech. J. 27, 379 and 623 (1948).
  3.  T. M. Cover, J. A. Thomas, Elements of Information Theory 
(Wiley, New York, ed. 2, 2006).
  4.  R. Cheong, A. Rhee, C. J. Wang, I. Nemenman, 
A. Levchenko, Science 334, 354 (2011); 10.1126/
science.1204553.  
  5.  F. Rieke, D. Warland, R. de Ruyter van Steveninck, 
W. Bialek, Spikes: Exploring the Neural Code (MIT Press, 
Cambridge, MA, 1999).
  6.  T. Berger, IEEE Inf. Theory Soc. Newsl. 53 (March 2003).
  7.  H. Barlow, in Sensory Communication, W. A. Rosenblith, 
Ed. (MIT Press, Boston, MA, 1961), pp. 217234.
  8.  B. A. Olshausen, D. J. Field, Nature 381, 607 (1996).  
  9.  E. C. Smith, M. S. Lewicki, Nature 439, 978 (2006).  
 10.  I. Lestas et al., Nature 467, 174 (2010).  
 11.  Y. M. Kabanov, Theory Probab. Appl. 23, 143 (1978).  
 12.  C. A. Parent, P. N. Devreotes, Science 284, 765 (1999).  
 13.  B. W. Andrews, P. A. Iglesias, PLOS Comput. Biol. 3, e153 
(2007).  
 14.  J. M. Kimmel, R. M. Salter, P. J. Thomas, Adv. Neural Inf. 
Process. Syst. 19, 705 (2007).
 15.  D. Fuller et al., Proc. Natl. Acad. Sci. U.S.A. 107, 9656 
(2010).  
Receiver   Destination
Noise
source
Signal   Received
signal
Message Message
Information
source
  Transmitter
Information  flow.  Schematic  diagram  of  a  general  communication  system  (  2).  The  information  capacity  of  a 
signaling system quanties its ability to transmit information (measured in bits), whether it is an engineered cable or 
a living cell. 
10.1126/science.1213834 C
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Globalization,   Land  Use,   and  the
Invasion  of   West   Nile  Virus
A.  Marm  Kilpatrick
Many  invasive  species  that  have  been  spread  through  the  globalization  of  trade  and  travel  are
pathogens.  A  paradigmatic  case  is  the  introduction  of  West  Nile  virus  (WNV)  into  North  America
in  1999.  A  decade  of  research  on  the  ecology  and  evolution  of  WNV  includes  three  findings
that  provide  insight  into  the  outcome  of  future  pathogen  introductions.  First,  WNV  transmission
in  North  America  is  highest  in  urbanized  and  agricultural  habitats,  in  part  because  the  hosts
and  vectors  of  WNV  are  abundant  in  human-modified  areas.  Second,  after  its  introduction,
the  virus  quickly  adapted  to  infect  local  mosquito  vectors  more  efficiently  than  the  originally
introduced  strain.  Third,  highly  focused  feeding  patterns  of  the  mosquito  vectors  of  WNV  result
in  unexpected  host  species  being  important  for  transmission.  This  research  provides  a  framework
for  predicting  and  preventing  the  emergence  of  foreign  vector-borne  pathogens.
T
he  growth  of  human  populations  and  the
development   of  rapid  transportation  sys-
tems  have  made  the  worlds  biota  more
connected than at any time in Earths history. The
result   has  been  a  breakdown  in  biogeographic
barriers and the introduction of species into nov-
el  habitats.   Globally,   introduced  invasive  spe-
cies  are  estimated  to  cause  >$120  billion  in
damage  annually  (1)  and  include  several  patho-
gens  that   have  direct   impacts  on  the  health  of
humans, livestock, and wildlife. Pathogens spread
by trade and travel in the past 500 years include
those causing the human diseases malaria, dengue,
and HIV/AIDS; wildlife and livestock pathogens,
such as anthrax, rinderpest, rabies, and avian ma-
laria;  and  numerous  diseases  of  crops  and  wild
plants,   including  chestnut   blight,   potato  blight,
and sudden oak death (2,   3). Introductions have
continued  with  invasions  by  novel   strains  of  in-
fluenza,  severe  acute  respiratory  syndrome,   and
West Nile virus (WNV), among many others. The
factors that determine the outcome and impact of
invasions are frequently complex and poorly un-
derstood  (4,   5);   however,   extensive  research  on
WNVover the past decade has enabled a detailed
exploration of its invasion, including pathways of
introduction, interactions with the biotic and abi-
otic environment in the new region (Fig. 1), and
impacts on ecosystem health.
WNV is  a  single-stranded  RNA virus  in  the
family  Flaviviridae  that  includes  several  impor-
tant humans pathogens: dengue, Japanese enceph-
alitis,   and  yellow  fever   viruses  (6).   WNV  was
first   isolated  in  1937  from  a  febrile  patient   in
Uganda, and subsequent studies showed that WNV
transmission was endemic and widespread across
tropical parts of Africa, southern Asia, and north-
ern  Australia,   and  episodic  in  more  temperate
parts  of  Europe  (7).  As  with  other  vector-borne
diseases,  the  warmer temperatures in the  tropics
facilitate longer transmission seasons and some-
times increased  transmission  intensity  through
faster  mosquito  and  virus  development   and  in-
creased  biting  rates.  In  some  populations  in  Af-
rica,   >80%  of  people  over  15  years  old  have
antibodies   to  WNV  (8);   however,   WNV  was
previously  considered  nearly  asymptomatic  and
in  the  1950s  was  even  tried  as  an  anticancer
therapy (9).
In  1999,   WNV  was   introduced  into  North
America, where it spread rapidly with major ec-
onomic and public health consequences (7). The
virus  reached  the  west   coast   in  only  4  years
(Fig.  2),   with  regional  epidemics  in  2002  and
2003 and more localized epidemics occurring in
other  years.  Between  1999  and  2010,  ~1.8  mil-
lion   people   were   infected,   with   ~360,000   ill-
nesses,   12,852   reported   cases   of   encephalitis/
meningitis, and 1308 deaths. The threat of WNV
infection has led to the costly implementation of
national  blood  donor  screening,  as  well  as  vac-
cine  and  drug  development   (10).   Public  out-
reach campaigns have altered human behavior,
including  the  time  spent   outdoors,   especially
by older   people, who are at high risk for WNV
disease.
The  impacts  of  WNVon  wildlife  have  been
yet more severe than those on humans. Millions
of   birds  have  died  from  WNV  infection,   and
regional-scale population declines of >50% have
been observed for several species (11). The range
of taxa that have suffered declines is surprisingly
large  and  includes  corvids,   chickadees  and  tit-
mice, wrens, and thrushes (Fig. 1) and probably
others.   Some  populations   have  recovered  after
initial declines, whereas others have not (11). The
REVIEW
Department   of   Ecology  and  Evolutionary  Biology,   Univer-
sity   of   California,   Santa   Cruz,   CA   95064,   USA.   E-mail:
akilpatr@ucsc.edu
Fig. 1. An American robin (T. migratorius) and its nestlings. Robins flourish in human-altered landscapes
and appear to play a key role in WNV amplification across many regions of North America. [Photo credit:
Bruce Lyon]
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   323
ecological  and  economic  consequences  of  these
regional declines in bird populations have not yet
been elucidated and need further study.
Globalization and the Introduction of Pathogens
The probability of the introduction and establish-
ment   of   introduced  species  has  been  shown  to
increase  with  the   propagule  pressure,  or   the
rate at which individual organisms are introduced
to a newregion (Fig. 3) (5). The yearly propagule
pressure and the pathway by which WNVreached
North  America   in  1999  remain  unknown,   but
several possibilities have been proposed, including
mosquitoes   being  transported  by  shipping,   air-
planes, or wind; migratory birds or birds in trade;
and humans traveling (12). The large and increas-
ing volume of air traffic into NewYork City over
the  past  five  decades  makes  the  transport  of  in-
fected  mosquitoes  on  an  airplane  a  likely  path-
way.  A  close  phylogenetic  relationship  between
viruses isolated in New York in 1999  and  those
circulating  in  Israel   in  the  previous  year   sug-
gests  a  possible  Middle  East   origin  (6).   Trade
and travel have also previously introduced key
mosquito  vectors  of  WNV,   Culex  pipiens  and
C.   quinquefasciatus,  as  well  as  vectors  for  den-
gue, yellow fever, and chikungunya viruses, such
as  Aedes  albopictus and  A.  aegypti (13).
What   predictions  could  have  been  made  in
1999  about   the  outcome  of  the  introduction  of
WNVinto New York City that summer? An an-
swer comes fromcomparing the ecology of WNV
transmission in the Americas with that in Africa
and Europe (14,  15).
WNV  Ecology  in  Its  Native  Range
Studies of endemic WNV transmission in Egypt,
Sudan,  and  South  Africa  and  of  Kunjin  virus,  a
subtype of WNV, in Australia showthat the virus
was most frequently isolated fromCulex mosqui-
toes.   In  Australia,   most   isolations  come  from
C. annulirostris, which is a competent laboratory
vector (16). In Africa, C. univittatus makes up the
largest   fraction  of   WNV-infected  mosquitoes
(8,   17).   Interestingly,   there  is  little  evidence  of
WNVinfection in  C.  pipiens in South Africa, de-
spite frequent feeding on avian hosts. C. pipiens is
an  important  WNV  vector  in  Europe  and  North
America  (15,   18).   It   is  possible  that   the  lower
WNVinfection prevalence observed in C. pipiens
than in C. univittatus can be attributed to its being
less susceptible to infection (17).
Accurate quantification of the contribution of
different   host   species  to  viral   amplification  re-
quires data on mosquito feeding patterns and host
abundance  from  the  same  place  and  time,  com-
bined  with  information  on  the  duration  and  in-
tensity of host infectiousness (19). Host abundance
and mosquito feeding data have never been col-
lected  simultaneously  for  WNV  hosts  and  vec-
tors in Africa, Asia, Australia, or Europe and have
only rarely been collected in North America. As a
result,   only  tentative  conclusions  can  be  drawn
about the relative importance of host species for
WNV outside  North  America  and  these  largely
come  from  studies  of  seroprevalence  and  infec-
tiousness based on viremia (concentration of virus
in  the  blood)  observed  after  experimental  infec-
tions. In Egypt, hooded crows (Corvus  cornix)
and  house  sparrows  (Passer   domesticus)   had
high antibody prevalence and infectiousness (8).
In South Africa, waterbirds (ducks and rails) and
passerine birds in the family Ploceidae (weavers
and  Old  World  sparrows,  including  house  spar-
rows) were most  infectious  and  most  frequently
had antibodies to WNV (17).
The  Vectors,  Hosts,  and  Transmission
of  WNV  in  the  Americas
The  most   important   vectors  in  North  America
share some similarities with those in Africa, Eu-
rope, and Australia. Although C. univittatus is not
present  in the Americas,   C.  pipiens,   C.   quinque-
fasciatus,  and  several  other  species  that  take  the
majority  of   their   blood  meals   from  birds  are
found  in  North  America,  including  C.   restuans,
C.   tarsalis,   and  C.   nigripalpus.   Based  on  their
feeding ecology and their vector competence, all
these species would be expected to be important
in  enzootic  (bird-to-bird)  transmission  (18,   20).
In addition, their abundance in anthropogenically
modified areas points to a significant role in hu-
man WNVepidemics.
An important insight was gained in the course
of determining the vector species responsible for
transmitting  WNV  from  nonhuman  animals  to
humans  (i.e.,   bridge  vectors).   Bridge  vectors
were initially thought to be mosquito species that
fed frequently on mammals (such as  Aedes mos-
quitoes),  but  an  integrated  analysis  of  the  abun-
dance, infection prevalence, feeding patterns, and
vector competence of a wide range of mosquitoes
indicated  that   C.   pipiens  and  C.   restuans  mos-
quitoes, which frequently take <15%of their blood
meals from humans, may nonetheless be respon-
sible for the majority of human infections in sev-
eral regions (18, 21). Their importance results from
their  higher  relative  abundance  and  WNV infec-
tion  prevalence than the more anthropophilic mos-
quito species. Applying this integrated approach
to other pathogens may simplify targets for vec-
tor control, especially when the same species serves
as both the bridge and the enzootic vector.
0
47
0.0
0.2
0.4
0.6
0.8
1.0
Not detected yet
1999
2000
2001
2002
2003
2004
2005
2007
2009
1   2   3   4   5   6   7   8   9   10   11
Years since WNV detection in that state
Years of WNV 
detection
R
e
l
a
t
i
v
e
 
n
u
m
b
e
r
 
o
f
 
c
a
s
e
s
47 47 47 47 47 47 46 43 27 12 4
Fig. 2. Spread of WNV throughout the Americas. The map shows the year that WNV was first detected in a
state, province, or country. The box plot shows the temporal pattern of WNV incidence at the state level
after WNV arrival. The y axis shows the relative number of WNV neuroinvasive cases (the fraction of the
maximum observed in that state) that occurred in each state in each year, starting with the year WNV was
first detected in birds, mosquitoes, humans, or horses. The number of states included in each column is
shown above the box.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 324
REVIEW
Predicting  which  avian  hosts  would  be  im-
portant  for  WNV  transmission  in  the  Americas
based on data from Africa or Europe would have
failed, because inferences based solely on abun-
dance,   infectiousness,   or   serological   (antibody)
prevalence  can  be  misleading  (19).  Analyses  of
data from the mid-Atlantic to Colorado that have
combined host abundance and mosquito feeding
data  with  host   infectiousness  suggested  that   al-
though introduced house sparrows (P. domesticus)
and  crows   (Corvus   spp.)   are   abundant   and/or
highly infectious, they appear to be of minor im-
portance  in  WNV  transmission  (2123).  Crows
make up a small fraction of mosquito blood meals,
and  house  sparrows  are  rarely  fed  on  by  mos-
quitoes  relative  to  their  abundance,   resulting  in
few  bites   per   individual   and  inefficient   trans-
mission.  Instead,  a  species  of  thrush,  the  Amer-
ican  robin  (Turdus   migratorius),   appears  to  be
more  important   in  WNV  transmission  (Fig.   4)
(2123). This is primarily because 30 to 80% of
mosquito  feedings  by  the  dominant  WNV vec-
tors (C. pipiens, C. restuans, and C. tarsalis) are on
robins, despite robins making up only 1 to 20%
of   the  avian  communities   studied.   Questions
that  arise  are  why  are  robins  so  frequently  fed
on  by  mosquitoes,   and  do  robins  share  a  trait
with  other thrushes  that  makes  them  generally
important for avian arboviruses? For example,
serological studies of the avian Sindbis virus in
Sweden  indicated  higher  exposure  of  thrushes
than of any other group (24).
Research has also shown that focused feeding
on robins amplifies WNV transmission intensity
(22). This raises the following question: If Amer-
ican robins, which have increased 50 to 100% in
abundance  over   the  past   25  years  with  the  ur-
banization of the North American landscape (11),
were less abundant, would WNVtransmission be
lower? Its uncertain, because if mosquito abun-
dance  and  feeding  patterns  remain  constant,  de-
creasing host abundance increases the vector:host,
ratio  which  increases  transmission  intensity.   In
addition,  seasonal  decreases  in  robin  abundance
have been correlated with a shift in mosquito feed-
ing  from  birds  to  humans,   which  increases  hu-
man WNVinfections (25). However, in the western
and southern United States, where robins are less
abundant, they provide only a small fraction of
mosquito blood meals, and yet mosquito feeding
by  another  species,   C.   quinquefasciatus,  on  hu-
mans  is  no  greater   than  in  the  east   (26).   As  a
result, the impact of reducing robin abundance on
WNVtransmission is unknown and would proba-
bly depend on the identity, abundance, and infec-
tiousness  of  alternate  sources  of  mosquito  blood
meals.
In  summary,   three   important   insights   have
been gained in determining the amplification hosts
of WNVin North America. First, abundant hosts
Human land use
Urbanization, Agriculture
Globalization of trade & travel
Greenhouse gases
Increases in human
commensal vectors
and hosts
Travel
Trade in animals
Animal migration
Altered CO
2
,
temperatures,
and precipitation
Fig.   3.   Anthropogenic  processes  that  facilitate  the  introduction  and  es-
tablishment   of   novel   pathogens  and  increase  their   transmission.   Trade,
travel,   and  animal   movement   introduce  new  pathogens.   Climate,   hosts,
and  the  abundance  and  feeding  ecology  of  vectors  determine  establish-
ment  and  transmission  intensity.  Land  use  modifies  animal  communities
that  serve  as  hosts  and  vectors  for  pathogens,  and  climate  change  alters
pathogen and vector demographic rates. [Image credits: Google and Tele
Atlas   (aerial   photos);   Edward   Canda   (rice   paddy);   Photos8.com  (corn-
field); L. Hufnagel (air traffic map); Dori (dori@merr.info) (smokestacks);
Joe  Hoyt (left mosquito); Andrew Flemming (right mosquito); Richard Kuhn,
Purdue  Department   of   Biological   Sciences  (virus);   NASA  (clouds);   Marm
Kilpatrick  (others)]
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   325
REVIEW
may  be  fed  on  infrequently  by  vectors,  making
them less important in transmission. Second, the
importance of hosts may be determined more by
how frequently mosquitoes feed on them than by
variation in their infectiousness. Finally, variation
in  the  abundance  of   key  avian  hosts  can  have
unpredictable impacts on transmission, especially
to humans.
Hosts  and  Vectors  as  Ecological  Niches
for  Pathogens
Studies  of  WNV amplification  hosts  show  how
the  feeding  patterns   and  competence  of   insect
vectors  and  vertebrate  hosts  create  ecological
niches for introduced vector-borne pathogens. Char-
acterization of these niches can informpredictions
of  establishment  probability  for  pathogen  intro-
ductions  (19)  and  augment   projections  that   are
frequently  based  on  climatic  conditions  alone.
Such predictions can be used to guide manage-
ment   decisions   in  allocating  resources   toward
prevention  of  pathogen  introductions  (such  as
vaccine development and testing and quarantine
of imported animals). One example of the insight
gained from host and vector competence studies
comes  from an elegant  comparison of WNVand
St.   Louis  encephalitis  virus  (SLEV,   a  flavivirus
native to the Americas) by Reisen et al. (27), which
showed that WNV is more infectious in hosts to
biting  vectors  than  SLEV  and  explained  why
WNVepidemics are more severe than those caused
by SLEV.
Land  Use  and  WNV  Transmission
Recent evidence has suggested that at the county
scale in eastern and western North America, hu-
man WNVincidence increases with urbanization
and agriculture, respectively (28) (Figs. 3,4). This
may  result   from  the  habitats  used  and  human-
commensal nature of three important WNVmos-
quito vectors, C. pipiens, C. quinquefasciatus, and
C.  tarsalis, although the exact mechanisms acting
at  local  scales  are  not  yet  known.  Nevertheless,
the distribution of WNVindicates that it is similar
to other pathogens whose transmission is linked
with anthropogenic land use and increased abun-
dance of domesticated animals and human-tolerant
wildlife  species  (Figs.   3  and  4).   For  example,
H5N1 avian influenza emerged from poultry in-
tensification; rabies transmission in the Serengeti
is  maintained  by  domestic  dogs;   Lyme  disease
increases  with  the  fragmentation  of  forests  in
eastern  North  America;   and  yellow  fever,   den-
gue, and chikungunya viruses are all transmitted
by the anthropophilic mosquitoes  A.  aegypti and
A.  albopictus (2933). Perhaps ecologically based
land-use planning, combined with improved de-
velopment   and  sanitation,   could  reduce  contact
with and the abundance of human-commensal spe-
cies and hence transmission of their pathogens.
Coevolution  of Hosts,  Vectors,  and Pathogens
Rapid  coevolution  between  WNV and  its  hosts,
vectors,   and  other  pathogens  is  expected  based
on reciprocal fitness impacts and in many cases, the
lack of shared evolutionary history (11, 27, 34, 35).
Still,   it   was  somewhat   surprising  that   by  2005,
the strain of WNVthat was introduced into North
America  in  1999  (NY99)  had  been  displaced
continent-wide by a locally evolved genotype,
WN02  (36).  WN02  was  first  detected  in  2001
and  spread  continent-wide  between  2002  and
2004.  Viruses  in  the  WN02  clade  consistently
differ from NY99 viruses by only three nucle-
otides   that   result   in  one  amino  acid  change.
Nonetheless, WN02 viruses are more efficient-
ly transmitted by both  C.  pipiens and  C.  tarsalis
mosquitoes, and the difference was  found to in-
crease with temperature in the laboratory, as would
be  expected  if  the  WN02  viruses  replicate  at   a
higher rate (37,  38).
Fig. 4. WNV ecology across an urbanization gradient in the northeastern and
midwestern United States. WNV is transmitted primarily by C. pipiens mosqui-
toes  among  a wide  range  of  birds,  but  American  robins  (outlined)  are  a  key
amplification  host.   The  diversity  of  avian  hosts  decreases  with  urbanization,
whereas  C.  pipiens  abundance  appears  to  increase.  [Image  credit:  U.S.  Geo-
logical Survey (mosquito); Marm Kilpatrick and Ryan Peters (others)]
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 326
REVIEW
The difference between NY99 and WN02 vi-
ruses  in  competence  (that   is,   in  magnitude  and
duration of infectiousness) in avian hosts has not
yet   been  determined.   However,   another   single-
stranded RNAvirus, Venezuelan equine enceph-
alitis virus,  has  repeatedly evolved to be able to
infect novel hosts and mosquito vectors efficient-
ly,   and  this   shows   that   host   adaption  is   also
possible (33).
There may be evolutionary selective pressure
for WNV to kill its avian hosts. Individual birds
that   die   from  WNV  infection  have   higher   vi-
remia, and thus infectiousness to biting mosqui-
toes,  than  individuals  that  survive  (27,   34),  and
host   illness   from  infection  decreases   host   de-
fenses  against   biting  mosquitoes,   which  would
increase  vector-host  contact  rates.  Both  of  these
mechanisms   increase   pathogen   fitness   by   in-
creasing host-to-vector transmission. In addition,
in contrast to an assumption made in many mod-
els of the evolution of virulence, host death from
WNV  does  not  appear  to  reduce  the  length  of
the  infectious  period  of   the  host:   Most   avian
hosts  that   survive  WNV  infection  clear   virus
from  their blood between days 4 and 6 after in-
fection, and most individuals that die from WNV
infection  do  so  at  approximately  the  same  time
after infection (27, 34). Akey question is whether
viral  evolution  that  increased  replication and vi-
rulence in hosts would have deleterious effects
in the vector.
It  is  also  unknown  whether  North  American
birds have evolved increased resistance to WNV.
This could be determined by repeating WNVlab-
oratory  challenge  experiments  using  individuals
from  the  same  populations  in  which  resistance
was previously measured early in the WNVepi-
demic  (27,   34).   Ideally,   such  studies  would  in-
clude a range of host species or populations that
have   experienced   different   selective   pressures
exerted on them by WNV; for example, in terms
of WNV transmission intensity or initial suscep-
tibility to WNVmortality (for example, doves are
more resistant than corvids) (27,  34).
Outlook:   Unanswered  Questions
A  key  question  is  will  WNV  follow  the  boom-
and-bust  pattern  seen  in  some  plant  and  animal
species  invasions  (5)are  the  worst  WNV epi-
demics  behind  us?  WNV epidemics  peaked  in
many states the year after it arrived, with fewer
human cases having been observed subsequent-
ly (Fig. 2). This reduction in WNV disease has
led  to  reduced  research  focus  and  less  funding
from public health agencies for WNV, and, more
recently,   less   testing  for   WNV  by  health  care
providers.
Reduced  transmission  may  be  a  product   of
several   factors,   including  elevated  immunity  in
birds or humans, especially the subset of people
most   at   risk:   the  homeless  and  those  spending
more time outdoors at dusk (7). However, annual
recruitment of young-of-the-year birds apparent-
ly fuels WNV(39), which reduces the importance
of avian host immunity in suppressing transmis-
sion. Instead, its possible that WNVtransmission
is  modulated  primarily  by  rainfall   and  temper-
ature, and if so, climatic conditions in 2002 and
2003 were especially suitable. Climate is known
to influence many aspects of WNV transmission,
including  mosquito  abundance,   biting  rate,   and
survival   as  well   as  viral   replication  within  the
mosquito (37). If WNV transmission is regulated
by  climate,   then  severe  epidemics  could  recur,
especially if they are facilitated by climate change
(Fig.  3).  It  is  notable  that  the  largest  number  of
neuroinvasive WNVcases observed in NewYork
State  was  in  2010,  11  years  after  the  virus  was
introduced. Clearly, determining the relative roles
of  climate  versus  other  factors  in  year-to-year
variation in transmission is important and neces-
sary to predict the long-term trajectory of WNV
in North America.
Asecond unanswered question is why havent
more  morbidity  and  mortality  been  reported  in
horses,   humans,   and  birds  in  tropical   regions
(7,  40)? Less surveillance is undertaken in these
less-developed  countries  than  in  North  Amer-
ica, and the presence of other diseases, such as
dengue, malaria, and Chagas, whose public health
impact dwarfs that of WNV, could account for
lower reporting, despite similar WNVincidence
and illness. Alternatively, cross-protection by anti-
bodies or evolved resistance to illness from other
flaviviruses (such as SLEV, dengue, or yellow
fever viruses) in humans and horses may decrease
illness,   without   reducing  bird-mosquito  trans-
mission. In addition,  enzootic transmission may
be lower in the tropics than in North America,
owing to cross-protecting flavivirus  antibodies  in
birds,  a  mismatch  between  periods  of  peak  mos-
quito abundance and susceptible young-of-the-
year  birds,   or  lower  infectiousness  of  tropical
avian hosts. These mechanisms may be operating
simultaneously.
Continual   introduction  of  pathogens  to  new
regions  is  inevitable  in  our   globally  connected
planet. It is unclear which vector-borne pathogen
will be the next to cross hemispheres, but many
viruses  of  public  health  concern  exist  in  Africa,
Asia, and Europe, including other arthropod-borne
viruses such as Japanese encephalitis, Rift Valley
fever,   tick-borne  encephalitis,   and  chikungunya
(31). Conversely, there are several pathogens from
the  Americas  that   could  be  introduced  into  the
Old World, including Venezuelan equine enceph-
alitis  and  SLEV.   Insights  gained  from  studying
the invasion of WNV can be used to help predict
which  are  the  highest-risk  pathogens  for  estab-
lishment after cross-hemispheric introduction (19).
Gaining an understanding of the ecology of zoo-
notic viruses, combined with fast-developing re-
combinant vaccine technologies that have already
been applied to wildlife (41), could formthe basis
of a strategy to prevent the emergence of newly
introduced pathogens.
References  and  Notes
1.   D.   Pimentel,   R.   Zuniga,   D.   Morrison,   Ecol.   Econ.   52,
273  (2005).
2.   P.  K.  Anderson  et  al.,  Trends  Ecol.  Evol.  19,  535  (2004).
3.   P.   Daszak,   A.   A.   Cunningham,  A.   D.   Hyatt,   Science  287,
443  (2000).
4.   R.   N.   Mack  et  al.,   Ecol.   Appl.   10,  689  (2000).
5.   A.   K.   Sakai   et  al.,   Annu.   Rev.   Ecol.   Syst.   32,  305
(2001).
6.   R.   S.  Lanciotti   et  al.,   Science  286,   2333  (1999).
7.   L.   R.   Petersen,   E.   B.   Hayes,   Med.   Clin.   North  Am.   92,
1307,   ix  (2008).
8.   H.   S.   Hurlbut,   F.   Rizk,  R.   M.   Taylor,   T.  H.   Work,   Am.  J.
Trop.   Med.   Hyg.   5,   579  (1956).
9.   C.   M.  Southam,  A.   E.   Moore,   Am.   J.   Trop.   Med.   Hyg.
3,   19  (1954).
10.   D.   W.   C.   Beasley,   Immunotherapy  3,  269  (2011).
11.   S.   L.  LaDeau,   A.   M.   Kilpatrick,  P.   P.   Marra,   Nature  447,
710  (2007).
12.   A.   M.   Kilpatrick  et  al.,   Conserv.  Biol.   20,   1224  (2006).
13.   L.   P.   Lounibos,   Annu.   Rev.   Entomol.   47,  233  (2002).
14.   Z.   Hublek,   J.   Halouzka,  Emerg.   Infect.  Dis.   5,  643
(1999).
15.   M.  V.  Fyodorova  et  al.,  J.  Med.  Entomol.  43,  552  (2006).
16.   R. A. Hall, J. H. Scherret, J. S. Mackenzie, Ann.  N.Y. Acad.
Sci.   951,  153  (2001).
17.   B. M. McIntosh, P. G. Jupp, D. B. Dickinson, G. M. McGillivray,
J.  Sweetnam,  S.  Afr.  J.  Med.  Sci.  32,  1  (1967).
18.   A. M. Kilpatrick et al., Emerg. Infect. Dis. 11, 425 (2005).
19.   Supporting  material   is  available  on  Science  Online.
20.   M.   J.   Turell,   M.   R.   Sardelis,   M.  L.   O'Guinn,   D.   J.   Dohm,
in  Japanese  Encephalitis  and  West  Nile  Viruses  Vol.   267
Current  Topics  in  Microbiology  and  Immunology,
J. Mackenzie, A. Barrett, V. Deubel, Eds. (Springer-Verlag,
Berlin,   2002),  pp.   241252.
21.   G.   L.   Hamer  et  al.,   Am.   J.   Trop.   Med.   Hyg.   80,  268
(2009).
22.   A.   M.   Kilpatrick,   P.   Daszak,   M.   J.   Jones,   P.   P.   Marra,
L.   D.   Kramer,   Proc.   Biol.   Sci.  273,   2327  (2006).
23.   R.  Kent,  L.  Juliusson,  M.  Weissmann,  S.  Evans,  N.  Komar,
J.   Med.   Entomol.   46,   380  (2009).
24.   J.   O.   Lundstrm,   K.   M.  Lindstrm,   B.   Olsen,   R.   Dufva,
D.   S.   Krakower,   J.   Med.   Entomol.   38,  289  (2001).
25.   A.   M.   Kilpatrick,   L.   D.   Kramer,   M.  J.   Jones,   P.   P.   Marra,
P.   Daszak,   PLoS  Biol.   4,  e82  (2006).
26.   G. Molaei et al., Am. J. Trop. Med. Hyg. 83, 1269 (2010).
27.   W.   K.   Reisen,  Y.   Fang,   V.   M.   Martinez,   J.  Med.   Entomol.
42,  367  (2005).
28.   S.   E.  Bowden,   K.   Magori,   J.   M.  Drake,   Am.  J.   Trop.
Med.   Hyg.   84,  234  (2011).
29.   J.   L.   Kyle,   E.   Harris,   Annu.   Rev.   Microbiol.   62,  71
(2008).
30.   B.   F.   Allan,   F.   Keesing,   R.   S.   Ostfeld,   Conserv.   Biol.   17,
267  (2003).
31.   S. C. Weaver, W. K. Reisen, Antiviral Res. 85, 328 (2010).
32.   T.   Lembo  et  al.,   J.   Appl.   Ecol.   45,  1246  (2008).
33.   S.   C.  Weaver,   A.   D.   T.   Barrett,   Nat.  Rev.   Microbiol.   2,
789  (2004).
34.   N.   Komar  et  al.,   Emerg.   Infect.  Dis.   9,  311  (2003).
35.   J.   N.   Thompson,   Am.   Nat.   153,  S1  (1999).
36.   C.   T.   Davis  et  al.,   Virology  342,  252  (2005).
37.   A.  M.  Kilpatrick,  M.  A.  Meola,  R.  M.  Moudy,  L.  D.  Kramer,
PLoS  Pathog.   4,   e1000092  (2008).
38.   R.   M.   Moudy,   M.   A.   Meola,   L.  L.   Morin,   G.   D.   Ebel,
L.   D.   Kramer,   Am.   J.  Trop.  Med.   Hyg.   77,   365  (2007).
39.   G.   L.   Hamer  et  al.,   Vector  Borne  Zoonotic  Dis.   8,
57  (2008).
40.   N.   Komar,   G.  G.   Clark,   Pan  Am.   J.   Public  Health  19,
112  (2006).
41.   C.   A.   Russell,   D.   L.   Smith,   J.   E.  Childs,   L.   A.   Real,
PLoS  Biol.   3,  e88  (2005).
Acknowledgments:   I  thank  T.  Bogich,   K.   Koelle,   I.   Parker,
N.   Komar,   and  the  Kilpatrick  lab  for  input.   NSF  grants
EF-0914866  and  BCS-0826779  and  NIH  grant
1R01AI090159-01  provided  funding.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/323/DC1
SOM  Text
Fig.  S1
References
10.1126/science.1201010
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   327
REVIEW
The  Influence  of   Nonlinear
Mesoscale  Eddies  on  Near-Surface
Oceanic  Chlorophyll
Dudley  B.  Chelton,
1
*  Peter  Gaube,
1
Michael  G.   Schlax,
1
Jeffrey  J.  Early,
2
Roger  M.  Samelson
1
Oceanic  Rossby  waves  have  been  widely  invoked  as  a  mechanism  for  large-scale  variability  of
chlorophyll  (CHL)  observed  from  satellites.  High-resolution  satellite  altimeter  measurements  have
recently  revealed  that  sea-surface  height  (SSH)  features  previously  interpreted  as  linear  Rossby
waves  are  nonlinear  mesoscale  coherent  structures  (referred  to  here  as  eddies).  We  analyze  10  years
of  measurements  of  these  SSH  fields  and  concurrent  satellite  measurements  of  upper-ocean  CHL
to  show  that  these  eddies  exert  a  strong  influence  on  the  CHL  field,  thus  requiring  reassessment
of  the  mechanism  for  the  observed  covariability  of  SSH  and  CHL.  On  time  scales  longer  than  2
to  3  weeks,  the  dominant  mechanism  is  shown  to be  eddy-induced  horizontal  advection  of  CHL  by
the  rotational  velocities  of  the  eddies.
A
decade  of   concurrent   satellite  measure-
ments  of  sea  surface  height  (SSH)  and
upper-ocean  chlorophyll   (CHL)  is  en-
abling  studies  of  physical-biological  interaction
that are not feasible from ship-based observations.
Although satellites provide only near-surface in-
formation about ocean physics and biology, they
are the only practical means of obtaining dense,
global observations. Altimetric measurements of
SSH reveal that westward propagation is ubiqui-
tous  (1)  with  characteristics  similar  to  the  linear
Rossby waves by which the ocean adjusts to wind
and  thermal   forcing  (2).   Westward  propagation
is also evident in CHL estimates derived from sat-
ellite  measurements  of   ocean  color.   The  wide-
spread  interpretation  of  the  westward-propagating
SSH variations as Rossby waves led naturally to
interpretations  that   the  CHL  variations  are  also
induced  by  Rossby  waves  (35).
The  mechanism  for  Rossby  wave  influence
on CHL has been debated (49), in part because
of inconsistency in the lag between variations of
SSH and CHL. The most  widely accepted view
is  that  the  covariability  between  SSH  and  CHL
arises   from  cyclical   advection  of   CHL  by  the
horizontal  velocity field  associated  with  passing
Rossby  waves  (79).
The  prevailing  view  before  the  recent  focus
on Rossby wave influence was that CHL concen-
tration is influenced by nonlinear eddies (1015).
Investigations  of  this  eddy  influence  have  con-
tinued  in  parallel   with  Rossby  wave  studies.
Here, we show that the copropagation of CHL
and  SSH  previously  interpreted  as  having  been
caused  by Rossby waves  is in  fact  attributable
to eddies.
Nonlinearity   of   SSH   variability.   High-
resolution  SSH  fields  produced  by  merging  the
measurements  from  two  simultaneously  operat-
ing satellite altimeters (16) reveal that westward-
propagating  features   previously  believed  to  be
linear Rossby waves are actually nonlinear rotat-
ing  coherent   structures  (eddies)   with  radii   of
~100 km (17,  18). Because such mesoscale fea-
tures   propagate   westward   with   approximately
the speed of long Rossby waves (1719), they can
masquerade  as  Rossby  waves  in  low-resolution
SSH fields constructed from measurements by a
single  altimeter.
The degree of nonlinearity of a mesoscale fea-
ture is characterized by the ratio of the rotational
fluid  speed  U  to  the  translation  speed  c  of  the
feature.  When  U/c  >  1,  the  feature  is  nonlinear,
which  allows  it  to  maintain  a  coherent  structure
as  it   propagates  (20).   This  requires  that   all   of
the wavelength components of the feature prop-
agate at the same speed, i.e., nondispersively. With
linear  Rossby  wave  dynamics,   features  that   are
initially  spatially  compact  quickly  lose  their  co-
herent  structure  through  dispersion  (21).
At latitudes higher than 25, 98% of the fea-
tures  tracked  for   10  weeks  have  U/c  >  1  (fig.
S2). The degree  of  nonlinearity  is  slightly  less
at  lower  latitudes  where  the  propagation  speeds
c are faster (17,  18). But even in the latitude range
15  to  25,   95%  of  the  tracked  features  have
U/c  >  1  (fig.   S2).
Westward copropagation of SSH and CHL.
The revised interpretation of westward-propagating
SSH as nonlinear eddies mandates a reassessment
of  past   conclusions  that   the  westward  copropa-
gation of CHL and SSH is indicative of Rossby
wave  influence  on  CHL.   The  alternative  hy-
pothesis that CHL variability is eddy-induced is
examined here from 10 years of concurrent mea-
surements  of  SSH  and  CHL  in  the  southeastern
Pacific (SEP) near 20S that has been a focus of
past  studies  (6,   7).
The  trajectories  of  mesoscale  eddies  (18)  in
the  SEP  are  shown  in  Fig.  1A.  Compared  with
eddies   observed  globally  in  the   latitude   range
15 to 25, their mean amplitude is smaller (3.2 cm
versus 6.2 cm) but their mean radius is the same
(110  km).   Because  U  is  approximately  propor-
tional  to  eddy  amplitude,  eddies  in  the  SEP  are
less  nonlinear  (fig.  S2);  87%  have  U/c  >  1.
The mean CHL distribution has a generally
northward  gradient  over  most  of  the  SEP  (Fig.
1B). The influence of eddies is evident from the
sinuous  character  of  the  CHL  field  at   any  par-
ticular  time  (Fig.  1,  C  and  D).  The  distortions
of   an  otherwise  smoothly  varying  CHL  field
are  most   apparent   in  regions   of   strong  CHL
gradient.
Eddy  influence  on  the  CHL  field  becomes
clearer after filtering to remove the large-scale
and seasonally varying CHL and SSH (22). West-
ward copropagation of CHL and SSH is apparent
from time-longitude plots of the resulting anom-
aly  fields  (Fig.  2,  A  and  B).  The  trajectories  of
the  centroids   of   clockwise  (CW)   and  counter-
clockwise  (CCW)  rotating  eddies  in  the  SEP  co-
incide,   respectively,   with  negative  and  positive
extrema of westward-propagating SSH (Fig. 2A).
The  positive  lag  of   maximum  positive  correla-
tion in Fig. 2C indicates that the SSH extrema at
the  eddy  centroids  lag  the  extrema  of  westward-
propagating  CHL  by  ~1  month   in   the   eastern
SEP, decreasing to ~0.5 month in the west. There
is a weaker negative correlation at negative lags
of  1  to  1.5  months.
Eddy influence on CHL. To interpret the lagged
correlations in Fig. 2C, anomaly CHL was com-
posite averaged  within  eddy  interiors  in a  trans-
lating and rotated coordinate system in which the
large-scale  CHL  gradient  vector  is  oriented  at  a
polar angle of 90 (22). The CHL anomaly com-
posites   consist   of   dipoles   with  opposing  signs
and with different orientations in CWand CCW
rotating  eddies   (Fig.   3A).   As  indicated  by  the
ratio  r in Fig. 3A, the dipoles are asymmetric in
both cases with larger magnitudes in the left half
of each composite, corresponding to the leading
half  of  these  westward-propagating  eddies.  The
displacements  from  the  eddy  centroid  are  smaller
for   these  primary  poles  than  for   the  secondary
poles of opposite sign in the trailing (right) halves
of  the  eddies  (see  also  fig.  S4).
The negative extremum  of SSH at the cen-
troids of CW rotating eddies in the SEP is strad-
dled by negative and positive poles of CHL to the
west  and  east,  respectively.  The opposite  occurs
in  CCW  rotating  eddies,   for  which  the  positive
extremum  of   SSH  at   the  centroids  is  straddled
by  positive  and  negative  poles  of  CHL  to  the
west   and  east,   respectively.   The  parallel   bands
of   positive   and  negative  lagged  correlations   in
Fig.   2C  thus  arise  from  a  combination  of  west-
RESEARCHARTICLES
1
College of Oceanic and Atmospheric Sciences, 104 COAS Ad-
ministration  Building,   Oregon  State  University,  Corvallis,   OR
973315503,   USA.
  2
Northwest  Research  Associates,   Post  Of-
fice  Box  3027,  Bellevue,  WA  98009,  USA.
*To   whom  correspondence   should   be   addressed.   E-mail:
chelton@coas.oregonstate.edu
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 328
ward  propagation  and  the  zonal   alignments  of
the  monopole  extrema  of  SSH  and  dipole  ex-
trema  of  CHL.
The geographical patterns of anomalous CHL
within  the  eddy  interiors  in  this  region  of   gen-
erally northward CHL gradient  are  indicative of
horizontal   advection  of   CHL  by  the  rotational
velocities  of the eddies. For CW rotating eddies
(Figs.   3A  and  4A,   top  panels),   the  northward
velocity in the western half of each eddy advects
low CHL from south to north, resulting in anom-
alously low  CHL in the northwest quadrant. The
southward  velocity  in  the   eastern  half   of   each
such eddy advects high CHL from north to south,
resulting in anomalously high CHL in the south-
east   quadrant.   The  opposite  rotational   sense  of
CCW rotating eddies (Figs.  3A  and 4A, bottom
panels)   results   in  anomalously  high  and  low
CHL  in  the  southwest  and  northeast  quadrants,
respectively.
The   importance   of   composite   averaging
the  CHL  in  a  rotated  coordinate  system  is  clear
from  Fig.   4,   A  and  B.   The  dipole  patterns  of
anomaly  CHL  result   from  a   combination  of
the   rotational   sense   of   the   eddies   and  the   di-
rection of the CHL gradient. These dipoles are
manifest   as  distortions  of  the  total   CHL  field
(Fig.  1,  C  and  D).
The  CHL  anomaly  within  the  trailing  half
of   the   eddy   is   generally   weaker   and   noisier
than within the leading half because the trailing
half   encounters   a   CHL   field   that   has   been
distorted  by  the  leading  half.   The  noisiness
of  the  secondary  poles  accounts  for  the  some-
what   weaker  negative  correlations  in  Fig.   2C,
as well as their smaller composite average mag-
nitudes compared with the primary poles (Fig. 3A).
Within  an  individual  eddy,  the  structure  of
the  dipole  of   anomaly  CHL  from  eddy-driven
advection  varies,   depending  on  the  strength
and  orientation  of   the  geographically  and  tem-
porally  varying  gradient   of   CHL,   the  degree
of   eddy  nonlinearity  U/c,   and  the  influence  of
other  eddies  that   have  recently  perturbed  the
CHL  field.   Past   confusion  about   geographi-
cal  and  temporal  variations  of the  lag relation-
ships   between  SSH  and  CHL  is   therefore  not
surprising.
Rotational   advection  of  CHL  by  eddies  is
reproduced  in  numerical  model  simulations  of
random westward-propagating eddies in a tracer
field with a northward gradient (22). The dipoles
of   anomalous   tracer   concentration   for   weakly
nonlinear eddies (Fig. 3B) are very similar to the
dipoles of observed CHL in Fig. 3A. The model
reproduces  the  asymmetry  of  the  magnitudes  of
the dipoles, as well as the smaller offset between
the  eddy  centroid  and  the  primary  pole  in  the
leading  halves  of  the  eddies  compared  with  the
secondary pole in the trailing halves. The higher
rotational velocities within strongly nonlinear ed-
dies  result   in  tracer   dipoles  with  larger   magni-
tudes  and  with  centers  advected  farther  around
the  eddy  interiors  (Fig.  3C).
Composite  averaging  separately  for  the  SEP
eddies east and west of 108W (figs. S3 and S5)
reveals   that   the   longitudinal   variations   of   the
couplet  of  positive  and  negative  lagged  correla-
tions  in  Fig.   2C  are  attributable  to  longitudinal
variations  of  the  structures  of  the  CHL  dipoles.
The shorter lag of maximum positive correlation
in  the  west   is   due   to  smaller   displacements
between  the  eddy  centroids  and  the  primary
poles  of   CHL  anomaly  in  the  leading  halves
of  the  eddies.   The  near-symmetry  of  the  lags
of positive and negative correlation bands in the
east  is  consistent  with  the  near-symmetric  dis-
placements  of  the  dipole  centers  from  the  eddy
centroids.
The   geographical   patterns   of   eddy-induced
CHL  anomalies   in  the  SEP  are  similar   to  the
patterns   found   in   other   regions   of   northward
gradient of CHL. Composite averages of anomaly
CHL  computed   globally   between   latitudes   of
15   and   45   are   shown   in   Fig.   3D  for   the
tracked eddies within regions of northward CHL
gradient   (22).   The   telltale   asymmetric   dipole
patterns   from  opposing  meridional   advection
in  opposite   halves   of   the   eddies   are   readily
apparent.
Anomaly CHL was composite averaged for
regions   of   generally  southward  CHL  gradient
by  rotating  the  translating  coordinate  system
Fig.   1.   Geographical   characteristics  of   observed
SSH and CHL in the SEP. (A) The trajectories from
a 16-year data record of eddies  that rotate clock-
wise  (CW,  blue  lines)  and  counterclockwise  (CCW,
red  lines),   with  the  starting  locations   shown  by
solid  circles.   (B)   The  10-year  average  log
10
(CHL)
for   CHL  in  units   of   mg  m
3
,   with  a  contour   in-
terval   of  log
10
(CHL)  =  0.1,   increasing  northward,
and with the thick line corresponding to log
10
(CHL) =
1.3.   (C)   An   example   map   for   7   March   2001
showing   log
10
(CHL)   in   color   with   contours   of
positive   and   negative   anomaly   SSH  (solid   and
dashed  lines,   respectively)   at   intervals   of   2  cm,
excluding  the  zero  contour.   (D)  The  same  as  (C),
except   showing  anomaly  SSH  in  color   with  con-
tours of log
10
(CHL) at the same interval as in (B).
The horizontal lines  in each panel are the  section
along which the time-longitude plots in Fig. 2 and
the  spectra  in  Fig.  5,  A  to  C,  were  computed.
A
B
C
D
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   329
RESEARCH  ARTICLES
so that the large-scale CHL gradient vector is
oriented at a polar angle of  90. The axes of
the   CHL  dipoles   in  these  composite  averages
(Fig.   3E)   are  rotated  ~180  relative  to  those
in  regions  of   northward  CHL  gradient.   These
mirrored  dipoles  still   have  larger   magnitude  in
the leading (left) half of the westward-propagating
eddies.
When  U/c  >  1,   fluid  is  trapped  within  the
eddy  interior  and  transported  along  the  eddy  tra-
jectory (20, 21). This nonlinear signal of sustained
transport of fluid trapped in the eddy core is not
A   B   C   D   E
Fig.  3. Composite averages of filtered fields in a rotated and normalized
coordinate  system  (22)  within  the  interiors  of  CW  (top  panels)  and  CCW
rotating eddies (bottom panels). (A)  log
10
(CHL) in the region 18S to 22S,
130W to 80W. (B) A tracer field in a model simulation seeded with weakly
nonlinear Gaussian eddies. (C) A tracer field in the model seeded with strongly
nonlinear   Gaussian  eddies;   (D)   log
10
(CHL)   globally  between  15  and  45
latitude  in  regions  of   northward  CHL  gradient.   (E)   log
10
(CHL)   globally  be-
tween 15 and 45 latitude in regions of southward CHL gradient. The outer
perimeter  of  each  circle  corresponds  to  twice  the  eddy  radius  scale  L
s
  (22).
The  vectors  in  each  panel   are  the  gradient  of  the  composite  average  SSH,
which  is   proportional   to  the  geostrophic  velocity.   The  number   N  of   eddy
realizations in the composite average and the magnitude r of the ratio of the
primary  pole  in  the  leading  (left)  half  of  each  composite  to  the  secondary
pole  in  the  trailing  (right)   half   are  labeled  on  each  panel.   The  estimated
95%  confidence  intervals  along  profiles  connecting  the  dipole  extrema  in
each  of  these  composite  averages  are  shown  in  fig.  S4.
Fig.   2.   Spatial   and  tem-
poral variability of filtered
SSH and log
10
(CHL) obser-
vations (22) along 20S be-
tween 130W and 80W.
Time-longitude sections of
westward-only propagation
over a 3-year portion of the
10-year  period  analyzed
here are shown for (A) SSH
with eddy tracks within  T2
of 20S overlaid (dashed and
solid lines for CW and CCW
rotating eddies, respectively);
(B) log
10
(CHL) with the same
eddy tracks overlaid; and (C)
the lagged cross-correlation
between log
10
(CHL) at time
t  and  SSH at time  t  +  lag,
calculated  over  the  full  10-year  data  record;  the  white  areas  correspond  to
correlations smaller than the estimated 95% significance level of 0.083 (22).
Positive lags correspond to log
10
(CHL) leading SSH, and the contour interval
is 0.2 with the zero contour omitted for clarity. Analogous time-longitude
sections  and  lagged  cross  correlations  are  shown  for  the  SSH  and  tracer
fields from a quasi-geostrophic model in fig. S6.
A   B   C
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 330
RESEARCH  ARTICLES
the  signature  revealed  in  the  CHL  observations
described  here.  The  extrema  of  the  dipole  CHL
features occur near the radius of maximum rota-
tional velocity that defines the outer edge of the
eddy core (21). As the westward-translating eddies
impinge  on  preexisting  CHL  gradients,   ambient
fluid  is  advected  part  way  around  the  portion  of
the  eddy  outside  of  the  core  region  of  closed
streamlines  in  the  translating  reference  frame
(20,  21).
Spectral   analysis   of   SSH  and  CHL.   Wave
numberfrequency  spectra  of   SSH  and  CHL
provide further evidence that the westward propa-
gation  of  CHL  is  induced  by  nonlinear  eddies.
The  nondispersive  character  of  nonlinear  eddies
implies that  the spectral  variance should  fall  ap-
proximately along a straight line in wave number
frequency space. In contrast, the spectral variance
for  linear  Rossby  waves  would  be  constrained  to
frequencies defined by their dispersion relation.
The  wave  numberfrequency  spectrum  of
SSH in the SEP (Fig. 5A) is clearly inconsistent
with  the   theoretical   Rossby  wave   dispersion
relation,   regardless  of  whether  the  classical  the-
ory  is  modified  to  account   for   effects  of   mean
currents  or  rough  bottom  topography.   Where-
as  the  dispersion  relations  from  these  theories
all flatten with increasingly negative wave num-
ber,   the   spectral   variance   of   observed   SSH
extends   to  higher   frequencies,   straddling  the
Fig.  5.  Zonal (east-west) wave numberfrequency
spectra. (A) Filtered SSH for 130W to 80W along
20S (see fig. S1 for SSH spectra along four other
zonal   sections).   (B)   SSH  for   Gaussian  approxima-
tions of each tracked eddy for 130W to 80W along
20S [different  color  bars  are  used  to  accommodate
the smaller variance of the Gaussian approximations
(23)].   (C)   Filtered  log
10
(CHL)   for   130W  to  80W
along 20S. (D) SSH from days 3000 to 15,000 of a
model   simulation  with  purely   linear   dynamics.   (E)
SSH  from  days  3000  to  15,000  of  a  model   sim-
ulation  with  nonlinear  quasi-geostrophic  dynam-
ics  (see  also  fig.  S7,  A  to  C).  (F)  A  tracer  field  in
the  same  model  simulation  as  in  (E)  (see  also  fig.
S7, D to F). The negative wave numbers correspond
to westward propagation. The units are cm for SSH,
log
10
  of   mg  m
3
for   CHL,   and  arbitrary   for   the
tracer  field.   The  straight   lines  are  the  mean  eddy
speeds from observed SSH [4.9 cm s
1
, (A) to (C)]
and  from  SSH  in  the  model   [4.3  cm  s
1
,   (D)   to
(F)].  The  curved  lines  correspond  to  the  dispersion
relations for linear Rossby waves from the classical
theory  for   a  flat   bottom,   no  mean  currents,   and
zero   meridional   (north-south)   wave   number   (2)
(solid),   a  theory  that   accounts   for   mean  currents
(25)   (dashed),   and   a   theory   for   rough   bottom
topography   and  no  mean  currents   (26)   (dotted).
The latter two are irrelevant to the SSH fields from
the flat-bottom model with no mean currents in (D)
to (F).
A   B   C
D   E   F
Fig.  4.  Schematic diagram of eddy-driven horizontal advection of
CHL for CW and CCW rotating eddies (top and bottom, respectively)
propagating  westward  in  regions  where  the  CHL  gradient   is  (A)
northward and (B) northeastward. An otherwise smooth contour of
CHL (dashed lines) is distorted by the rotational velocity field within
the eddy, as shown by the solid lines. Advection of CHL within the
large-scale  background  CHL  gradient   results  in  the  positive  and
negative CHL anomalies shown by the red and purple regions, re-
spectively. The dependence of the locations of these CHL anomalies
on the direction of the large-scale background CHL gradient that is
evident from comparison of (A) and (B) was accounted for by com-
posite averaging in a coordinate system rotated for each eddy (22).
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   331
RESEARCH  ARTICLES
straight  line  of  constant  (nondispersive)  prop-
agation  speed.
We   tested  our   hypothesis   that   the   spectral
characteristics of SSH in Fig. 5A are attributable
to  eddies  with  compact  structures  by  construct-
ing  SSH  fields  consisting  only  of  the  interiors
of  the  tracked eddies and zero outside of the ed-
dies.   Each  eddy  was   approximated  as   an  axi-
symmetric  Gaussian  feature with  amplitude  and
scale   estimated  from  the   automated  tracking
procedure  (18).  The  spectral  variance  of  the  re-
sulting  eddy-only  SSH  fields  (Fig.   5B)   strad-
dles  the  same  straight   line  as  the  spectrum  of
total SSH (23,  24). The discrepancies between
the wave numberfrequency spectra of SSH and
the  Rossby  wave  dispersion  relations   are  thus
consistent   with  SSH  variability  being  attributa-
ble  to  a  field  of  propagating  eddies.
The   importance   of   nonlinearity   is   clarified
from model simulations. The spectral variance of
model SSH with linear dynamics is restricted to
frequencies   below  the   dispersion   relation   for
Rossby  waves  with  zero  meridional  wave  num-
ber (Fig. 5D). The spread of variance to frequen-
cies  below  this  dispersion  relation  is  from  Fourier
components   with  finite  meridional   wave  num-
bers  (2).
With  nonlinear  quasi-geostrophic  dynamics,
the spectral variance of model SSH primarily rep-
resents long-lived, coherent eddy features, in which
the  small-scale  spectral   components  are  phase-
locked  to  the  large-scale  components  (21).   The
resulting  spectrum  (Fig.   5E)  consists  of  a  non-
dispersive band along a straight line that extends
to frequencies  higher than are  allowed  by linear
Rossby wave dynamics, very similar to the spec-
trum  of  observed  SSH  in  Fig.  5A.
A  short   spur  of  spectral  variance  centered
at about 0.007 cycles per day (cpd) extends along
the  dispersion  relation  in  the  model   SSH  spec-
trum  (Fig.   5E).   This   spur   arises   from  small-
amplitude  SSH  variability  outside  the  nonlinear
cores   of   the  eddies.   The  extent   of   the  spur   is
found  to  decrease  with  increasing  nonlinearity
of the eddies (fig. S7). Although not apparent in
the  spectrum  of   observed  SSH  in  Fig.   5A,   sug-
gestions  of  similar  spurs  exist   in  SSH  spectra  in
other  regions  (fig.  S1).
Determination  of  the  spectrum  of  CHL  var-
iability  is  more  challenging  than  for  SSH  (22).
The  spectrum  of  CHL  in  the  SEP  (Fig.  5C)  is
nonetheless  similar  to  the  spectrum  of  SSH.  In
particular,   the  spectral   variance  is  concentrated
along   the   same   straight   line   of   nondispersive
variability  to  higher  frequencies  than  are  allowed
by  linear  Rossby  waves  theories.  Moreover,  the
spectral variance is restricted to smaller negative
wave   numbers   than  would  be   the   case   if   the
CHL  variability  were  induced  by  linear  Rossby
waves. A short spur of spectral variance straddles
the  dispersion  relation  at   about   0.008  cpd  for
the  same  reason  discussed  above  for  the  model
SSH  spectra.  Similar  spurs  are  found  in  spectra
of  tracer  fields  in  quasi-geostrophic  model  sim-
ulations  (Fig.   5F  and  fig.   S7,   D  to  F).   The  re-
stricted  wave  number  extents  of  these  spurs  are
an  important  distinction  from  the  spectral   char-
acteristics in Fig. 5D  that  would be found if the
CHL  or   tracer   variability   were   attributable   to
linear  Rossby  waves.
Conclusions. Westward copropagation of CHL
and SSH that has previously been attributed to
linear Rossby waves is actually caused by non-
linear eddies that were not resolvable in the SSH
fields  analyzed  in  past  studies.  This  eddy  influ-
ence is manifest as distortions of the CHL field
and  is  most  evident  in  regions  of  strong  gradi-
ents of the CHL field. Eddy influence on CHL
becomes  clearer   after   filtering.   The  distinctly
different dipole structures of the resulting anom-
alous  CHL  distribution  within  the  interiors  of
CW  and  CCW  rotating  eddies  (Fig.   3,   A,   D,
and  E)  and  their  similarity  to  the  dipoles  of  a
tracer field in model simulations (Fig. 3, B and C)
are evidence that the dominant mechanism  for
eddy-induced CHL variability on the time scales
>2 to 3 weeks considered here (22) is horizontal
advection of CHL by the rotational velocity with-
in  the  interior  of  each  eddy.
The   dominance   of   horizontal   advection  as
the mechanism for the observed westward prop-
agation  of   CHL  variability  has  been  suggested
previously (79) but has been attributed to hori-
zontal  advection by linear Rossby waves, rather
than  to  nonlinear  eddies.  [The  role  of  eddies  in
defining  the  dipole  structure  of  CHL  anomalies
has   been  suggested  for   the   central   North  At-
lantic  (14,   15).]   The  distinction  between  linear
Rossby  waves  and  eddies  is  important   because
the  dynamics   of   nonlinear   eddies   differ   fun-
damentally  from  those  of  linear  Rossby  waves.
While   distinct   from  the   rotational   advection
identified   here,   eddies   can   trap   and   transport
fluid parcels and their associated water proper-
ties (20,  21), including nutrients, CHL, and zoo-
plankton. They can also upwell nutrient-rich water
by  various  mechanisms  (1015),   thus  stimulat-
ing  the  growth  of  phytoplankton  and  increasing
CHL  in  the  eddy  core.   Such  eddy-induced  en-
hancements often occur deep in the euphotic zone
where  they  can  be  undetectable  in  the  satellite-
based measurements of near-surface ocean color
(1215).
Because  of   the  unique  trapping  of   fluid  in
the  cores  of  nonlinear  eddies,   it  is  perhaps  sur-
prising that the CHL distribution associated with
the  eddies  consists  of  dipoles  with  extrema  out-
side of the eddy cores, rather than monopoles of
positive  or  negative  CHL  anomalies  trapped  at
the eddy centers. Monopole structures with very
active  physical-biological   interaction  are  some-
times observed within eddy cores. In contrast to
the   ubiquitous   presence   of   rotational   advec-
tion around the outer portion of the eddies iden-
tified  here,   however,   such  monopole  structures
are usually episodic, often with time scales short-
er  than  the  2-  to  3-week  filtering  applied  here.
Although  it   is   unclear   whether   the  rotational
advection that dominates the variability on longer
time scales has important biological consequences,
the  results  presented  here  clarify  the  dynamical
importance   of   eddies   to   the   observed   CHL
distribution.
References  and  Notes
1.   D.  B.  Chelton,  M.   G.   Schlax,  Science  272,  234  (1996).
2.   A.  E.  Gill,   Atmosphere-Ocean  Dynamics  (Academic  Press,
Cambridge,   1982).
3.   P.  Cipollini,  D.  Cromwell,  P.  G.  Challenor,  S.  Raffaglio,
Geophys.   Res.   Lett.   28,   323  (2001).
4.   B. M. Uz, J. A. Yoder, V. Osychny, Nature 409, 597 (2001).
5.   D.   A.   Siegel,   Nature  409,   576  (2001).
6.   Y.   Dandonneau,   A.   Vega,   H.   Loisel,  Y.   du  Penhoat,
C.   Menkes,   Science  302,   1548  (2003).
7.   P.   D.   Killworth,   P.   Cipollini,  B.   M.   Uz,   J.   R.   Blundell,
J.   Geophys.   Res.   109,  C07002  (2004).
8.   G.   Charria  et  al.,   J.   Mar.   Res.   64,  43  (2006).
9.   E.   Gutknecht,   I.   Dadou,   G.   Charria,
P.   Cipollini,   V.   Garon,   J.   Geophys.   Res.   115,
C05004  (2010).
10.   P.   G.   Falkowski,   D.   Ziemann,  Z.   Kolber,  P.   K.   Bienfang,
Nature  352,  55  (1991).
11.   D.  J.  McGillicuddy  Jr.  et  al.,  J.  Geophys.  Res.  104,  13381
(1999).
12.   D.   A.   Siegel,   D.   J.   McGillicuddy  Jr.,   E.   A.   Fields,
J.   Geophys.   Res.   104,  13359  (1999).
13.   D.  J.  McGillicuddy  Jr.  et  al.,  Science  316,  1021  (2007).
14.   D.   A.   Siegel   et  al.,   Deep  Sea  Res.   Part  II   Top.   Stud.
Oceanogr.   55,  1218  (2008).
15.   D.   A.   Siegel,   P.   Peterson,   D.   J.   McGillicuddy  Jr.,
S.   Maritorena,   N.  B.   Nelson,   Geophys.   Res.  Lett.   38,
L13608  (2011).
16.   N.   Ducet,   P.-Y.   Le  Traon,   G.   Reverdin,   J.  Geophys.   Res.
105,   19477  (2000).
17.   D.   B.  Chelton,  M.   G.   Schlax,   R.   M.   Samelson,
R.  A.   de  Szoeke,  Geophys.  Res.  Lett.   34,  L15606  (2007).
18.   D.   B.  Chelton,  M.   G.   Schlax,   R.   M.   Samelson,   Prog.
Oceanogr.   91,  167  (2011).
19.   J.  C.  McWilliams,  G.  R.  Flierl,  J.  Phys.  Oceanogr.  9,  1155
(1979).
20.   G.  R.  Flierl,  Geophys.  Astrophys.  Fluid  Dyn.  18,  39  (1981).
21.   J. J. Early, R. M. Samelson, D. B. Chelton, J. Phys. Oceanogr.
41,  1535  (2011).
22.   Information on  methods  is  available as  supporting  online
material   on  Science  Online.
23.   The  somewhat  smaller  variance  is  due  to  unavoidable
biases  in  the  amplitudes  of  compact  mesoscale
features  as  estimated  by  the  automated  procedure  (18).
24.   The  large  spectral   variance  at  small   wave  numbers
(long  wavelengths)  in  the  spectrum  of  eddy-only  SSH
fields  is  easily  understood  qualitatively  from  consideration
of  a  single  Gaussian  eddy.   Because  the  Fourier
transform  of  a  Gaussian  in  space  is  a  Gaussian  in  wave
number,   the  associated  spectrum  is  dominated  by
variance  at  small   wave  numbers.   It  is  evident  from
Fig.   5B  that  this  dominance  of  spectral   variance  at
small   wave  numbers  for  a  single  Gaussian  feature  is
maintained  in  the  spectrum  of  a  superposition  of
many  Gaussian  eddies.
25.   P.   D.  Killworth,  D.  B.  Chelton,  R.  A.  de  Szoeke,  J.  Phys.
Oceanogr.  27,  1946  (1997).
26.   R. Tailleux, J. C. McWilliams, J. Phys. Oceanogr. 31, 1461
(2001).
Acknowledgments:   We  thank  D.  McGillicuddy  and  T.   Farrar
for  discussions  throughout  the  course  of  this  study.
We also  thank L.-L.  Fu, V. Combes, D. Siegel,  P. Cipollini,
E.   Shulenberger,   and  two  anonymous  reviewers  for
helpful   comments  on  the  manuscript.   This  research  was
supported  by  NASA  grants  NNX08AI80G  and
NNX08AR37G  and  NSF  Award  0621134.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1208897/DC1
Materials  and  Methods
Figs.   S1  to  S7
References
25  May  2011;   accepted  26  August  2011
Published  online  15  September  2011;
10.1126/science.1208897
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 332
RESEARCH  ARTICLES
Light   Propagation  with  Phase
Discontinuities:   Generalized  Laws  of
Reflection  and  Refraction
Nanfang  Yu,
1
Patrice  Genevet,
1,2
Mikhail  A.  Kats,
1
Francesco  Aieta,
1,3
Jean-Philippe  Tetienne,
1,4
Federico  Capasso,
1
*  Zeno  Gaburro
1,5
*
Conventional  optical  components  rely  on  gradual  phase  shifts  accumulated  during  light
propagation  to  shape  light  beams.  New  degrees  of  freedom  are  attained  by  introducing  abrupt
phase  changes  over  the  scale  of  the  wavelength.   A  two-dimensional  array  of  optical  resonators
with  spatially  varying  phase  response  and  subwavelength  separation  can  imprint  such  phase
discontinuities  on  propagating  light  as  it  traverses  the  interface  between  two  media.  Anomalous
reflection and refraction phenomena are observed in this regime in optically thin arrays of metallic
antennas  on  silicon  with  a  linear  phase  variation  along  the  interface,  which  are  in  excellent
agreement  with  generalized  laws  derived  from  Fermats  principle.  Phase  discontinuities  provide
great  flexibility  in  the  design  of  light  beams,  as  illustrated  by  the  generation  of  optical  vortices
through  use  of  planar  designer  metallic  interfaces.
T
he shaping of the wavefront of light with
optical   components  such  as  lenses  and
prisms, as well as diffractive elements such
as gratings and holograms, relies on gradual phase
changes accumulated along the optical path. This
approach is  generalized in transformation  optics
(1,   2),  which  uses  metamaterials  to  bend  light
in unusual ways, achieving such phenomena as
negative refraction, subwavelength-focusing, and
cloaking  (3,   4)  and  even  to  explore  unusual  ge-
ometries of space-time in the early universe (5).
A  new  degree  of  freedom  of  controlling  wave-
fronts can be attained by introducing abrupt phase
shifts over the scale of the wavelength along the
optical  path,   with  the  propagation  of  light  gov-
erned by Fermats principle. The latter states that
the trajectory taken between two points A and B
by a ray of light is that of the least optical path,
B
A
n(
r )dr, where n(
r )   accumu-
lated along the actual light path will be zero with
respect to infinitesimal variations of the path. We
show  that  an  abrupt  phase  shift   F(
r
s
)  over  the
scale of the wavelength can be introduced in the
optical path by suitably engineering the interface
between  two  media;   F(
r
s
)  depends  on  the  co-
ordinate
  
r
s
  along  the  interface.   Then,   the  total
phase  shift   F(
r
s
)   
B
A
k d
r  will  be  stationary
for the actual path that light takes;
k  is the wave
vector  of  the  propagating  light.  This  provides  a
generalization  of  the  laws  of  reflection  and  re-
fraction,  which  is  applicable  to  a  wide  range  of
subwavelength structured interfaces between two
media throughout the optical spectrum.
Generalized laws of reflection and refraction.
The  introduction  of   an  abrupt   phase  shift,   de-
noted as phase discontinuity, at the interface be-
tween two media allows us to revisit the laws of
reflection  and  refraction  by  applying  Fermats
principle. Consider an incident plane wave at an
angle  q
i
.   Assuming  that   the  two  paths  are  infi-
nitesimally close to the actual light path (Fig. 1),
then the phase difference between them is zero
k
o
n
i
sin(q
i
)dx  (F   dF)   
k
o
n
t
sin(q
t
)dx   F  0   1
where  q
t
 is the angle of refraction;  F and  F+dF
are, respectively, the phase discontinuities at the
locations where the two paths cross the interface;
dx is the distance between the crossing points;  n
i
and n
t
 are the refractive indices of the two media;
and  k
o
  =  2p/l
o
,   where  l
o
  is  the  vacuum  wave-
length. If the phase gradient along the interface is
designed  to  be  constant,   the  previous  equation
leads to the generalized Snells law of refraction
sin(q
t
)n
t
    sin(q
i
)n
i
  
  l
o
2p
dF
dx
2
Equation  2  implies  that  the  refracted  beam  can
have  an arbitrary  direction,  provided  that  a  suit-
able constant gradient of phase discontinuity along
the  interface  (dF/dx)  is  introduced.   Because  of
the nonzero phase gradient in this modified Snells
law, the two angles of incidence  Tq
i
 lead to dif-
ferent   values   for   the  angle  of   refraction.   As   a
consequence,  there  are  two  possible critical  an-
gles  for  total  internal  reflection,   provided  that
n
t
 <  n
i
:
q
c
   arcsin
  
n
t
n
i
l
o
2pn
i
dF
dx
   
  3
Similarly, for reflection we have
sin(q
r
)  sin(q
i
) 
  l
o
2pn
i
dF
dx
4
where  q
r
  is  the  angle  of  reflection.   There  is  a
nonlinear  relation  between  q
r
  and  q
i
,  which  is
markedly different from conventional specular re-
flection. Equation 4 predicts that there is always a
critical angle of incidence
q
c
   arcsin   1 
l
o
2pn
i
dF
dx
   
  5
above   which   the   reflected   beam  becomes
evanescent.
In the above derivation, we have assumed that
F is a continuous function of the position along
the interface; thus, all the incident energy is trans-
ferred into the anomalous reflection and refraction.
However, because experimentally we use an array
of   optically  thin  resonators  with  subwavelength
separation  to  achieve  the  phase  change  along
the  interface,  this discreteness implies  that there
are also regularly reflected and refracted beams,
which  follow  conventional   laws  of   reflection
and refraction (dF/dx = 0 in Eqs. 2 and 4). The
separation   between   the   resonators   controls
the  amount   of   energy  in  the  anomalously  re-
flected  and  refracted  beams.   We   have   also
assumed  that  the  amplitudes  of  the  scattered
radiation by each resonator are identical, so that
the reflected and refracted beams are plane waves.
In the next section, we will showwith simulations
which represent numerical solutions of Maxwells
1
School   of   Engineering  and  Applied  Sciences,   Harvard  Uni-
versity,   Cambridge,  MA  02138,   USA.
  2
Institute  for  Quantum
Studies   and  Department   of   Physics,   Texas   A&M  University,
College  Station,   TX  77843,   USA.
  3
Dipartimento  di   Fisica  e
Ingegneria dei Materiali e del Territorio, UniversitPolitecnica
delle Marche, via Brecce Bianche, 60131 Ancona, Italy.
  4
Lab-
oratoire  de  Photonique  Quantique  et  Molculaire,  Ecole  Nor-
male Suprieure de Cachan and CNRS, 94235 Cachan, France.
5
Dipartimento  di   Fisica,   Universit degli   Studi   di   Trento,   via
Sommarive 14, 38100 Trento, Italy.
*To   whom  correspondence   should   be   addressed.   E-mail:
capasso@seas.harvard.edu   (F.C.);   gaburro@seas.harvard.
edu  (Z.G.)
Fig.  1.  Schematics used to derive the generalized
Snells law of refraction. The interface between the
two  media  is  artificially  structured  in  order  to  in-
troduce  an  abrupt   phase  shift   in  the  light   path,
which  is  a  function  of  the  position  along  the  in-
terface.  F and  F + dF are the phase shifts where
the two paths (blue and red) cross the boundary.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   333
RESEARCH  ARTICLES
equationshow,   indeed,   one  can  achieve  the
equal-amplitude condition and the constant phase
gradient along the interface through suitable de-
sign of the resonators.
There is a fundamental  difference between the
anomalous refraction phenomena caused by phase
discontinuities  and  those  found  in  bulk  designer
metamaterials, which are caused by either negative
dielectric   permittivity   and   negative   magnetic
permeability  or  anisotropic  dielectric  permittivity
with  different   signs  of   permittivity  tensor   com-
ponents along and transverse to the surface (3,  4).
Phase response of optical antennas. The phase
shift between the emitted and the incident radia-
tion of an optical resonator changes appreciably
across a resonance. By spatially tailoring the geom-
etry of the resonators in an array and hence their
frequency  response,   one  can  design  the  phase
discontinuity  along  the  interface  and  mold  the
wavefront of the reflected and refracted beams in
nearly  arbitrary  ways.   The  choice  of   the  reso-
nators  is  potentially  wide-ranging,  from  electro-
magnetic cavities (9,  10) to nanoparticle clusters
(11,   12)  and  plasmonic  antennas  (13,   14).   We
concentrated on the latter because of their widely
tailorable optical properties (1519) and the ease
of fabricating planar antennas of nanoscale thick-
ness. The resonant nature of a rod antenna made
of  a  perfect  electric  conductor  is  shown  in  Fig.
2A (20).
Phase shifts  covering  the 0-to-2p range  are
needed  to  provide  full  control  of  the  wavefront.
To  achieve  the  required  phase  coverage  while
maintaining large scattering amplitudes, we used
the double-resonance properties of V-shaped an-
tennas, which consist of two arms of equal length
h  connected  at  one  end  at  an  angle  D  (Fig.  2B).
We  define  two  unit   vectors  to  describe  the  ori-
entation of a V-antenna:  along the symmetry axis
of the antenna and  perpendicular to   (Fig. 2B).
V-antennas  support   symmetric  and  antisym-
metric modes (Fig. 2B, middle and right), which
are excited by  electric-field components  along  
and  axes, respectively. In the symmetric mode,
the current distribution in each arm approximates
Fig.   2.   (A)   Calculated  phase  and  amplitude  of
scattered light froma straight rod antenna made of
a perfect electric conductor (20). The vertical dashed
line  indicates  the  first-order  dipolar  resonance  of
the antenna. (B) A V-antenna supports symmetric
and  antisymmetric  modes,   which  are  excited,   re-
spectively, by components of the incident field along
 and  axes. The angle between the incident po-
larization  and  the  antenna  symmetry  axis  is  45.
The  schematic  current   distribution  is  represented
by colors on the antenna (blue for symmetric and
red  for  antisymmetric  mode),   with  brighter  color
representing  larger currents. The direction of cur-
rent flow is indicated by arrows with color gradient.
(C) V-antennas corresponding to mirror images of
those in (B). The components of the scattered elec-
tric field perpendicular to the incident field in (B)
and (C) have a  p  phase difference. (D and E) An-
alytically  calculated  amplitude  and  phase  shift  of
the  cross-polarized  scattered  light  for  V-antennas
consisting of gold rods with a circular cross section
and with various length  h and angle between the
rods D at l
o
= 8 mm(20). The four circles in (D) and
(E)  indicate  the  values  of  h  and  D  used  in  exper-
iments.   The  rod  geometry  enables  analytical   cal-
culations of the phase and amplitude of the scattered
light,   without   requiring  the  extensive  numerical
simulations  needed  to  compute  the  same  quan-
tities for   flat antennas with a rectangular cross-
section,   as  used  in  the  experiments.   The  optical
properties of a rod and  flat antenna of the same
length  are  quantitatively  very  similar,   when  the
rod   antenna   diameter   and   the   flat   antenna
width  and  thickness   are  much  smaller   than  the
length (20). (F) Schematic unit cell of the plasmonic
interface  for  demonstrating  the  generalized  laws  of
reflection and refraction. The sample shown in Fig. 3A
is created by periodically translating in the x-y plane
the  unit   cell.   The  antennas  are  designed  to  have
equal   scattering   amplitudes   and   constant   phase
difference DF =p/4 between neighbors. (G) Finite-
difference time-domain (FDTD) simulations  of  the
scattered electric field for the individual antennas
composing  the array in (F). Plots show the scat-
tered electric field polarized in the x direction for
y-polarized  plane  wave  excitation  at  normal  in-
cidence  from  the  silicon  substrate.   The  silicon
substrate  is  located  at  z    0.  The  antennas  are  equally  spaced  at  a  sub-
wavelength separation  G/8, where  G is the unit cell length. The tilted red
straight line in (G) is the envelope of the projections of the spherical waves
scattered  by  the  antennas  onto  the  x-z  plane.   On  account  of  Huygenss
principle,  the  anomalously  refracted  beam  resulting  from  the  superposi-
tion  of   these   spherical   waves   is   then  a   plane   wave   that   satisfies   the
generalized Snells law (Eq. 2) with a phase gradient |dF/dx| = 2p/G along
the interface.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 334
RESEARCH  ARTICLES
that of an individual straight antenna of length
h (Fig. 2B, middle), and therefore the first-order
antenna  resonance  occurs  at   h    l
eff
/2,   where
l
eff
 is the effective wavelength (14). In the anti-
symmetric mode, the current distribution in each
arm  approximates  that  of  one  half  of  a  straight
antenna  of  length  2h  (Fig.   2B,   right),   and  the
condition  for   the  first-order   resonance  of   this
mode is 2h    l
eff
/2.
The  polarization  of   the  scattered  radiation
is  the  same  as  that   of  the  incident   light   when
the  latter  is  polarized  along    or  .   For  an  ar-
bitrary incident polarization, both antenna modes
are  excited  but   with  substantially  different   am-
plitude and phase because of their distinctive reso-
nance conditions.  As a result, the scattered light
can have a polarization different from that of the
incident   light.   These  modal   properties  of   the
V-antennas  allow  one  to  design  the  amplitude,
phase, and polarization state of the scattered light.
We  chose  the  incident  polarization  to  be  at  45
with respect to  and  so that both the symmetric
and  antisymmetric  modes  can  be  excited  and
the  scattered  light   has  a  substantial   component
polarized orthogonal to that of the incident light.
Experimentally,  this  allows us to use  a polarizer
to decouple the scattered light fromthe excitation.
As  a  result   of  the  modal   properties  of  the
V-antennas and the degrees of freedomin choosing
antenna  geometry  (h  and  D),   the  cross-polarized
scattered  light  can  have  a  large  range  of  phases
and  amplitudes  for  a  given  wavelength  l
o
;  ana-
lytical   calculations  of   the  amplitude  and  phase
response  of  V-antennas  assumed  to  be  made  of
gold  rods are shown  in  Fig.  2,  D  and E.  In  Fig.
2D, the blue and red dashed curves correspond to
the  resonance  peaks  of  the  symmetric  and  anti-
symmetric  modes,   respectively.   We  chose  four
antennas  detuned  from  the  resonance  peaks,   as
indicated  by  circles  in  Fig.   2,   D  and  E,   which
provide an incremental phase of  p/4 from left to
right   for  the  cross-polarized  scattered  light.   By
simply taking the mirror structure (Fig. 2C) of an
existing  V-antenna  (Fig.  2B),  one  creates  a  new
antenna whose cross-polarized radiation has an ad-
ditional  p phase shift. This is evident by observing
that the currents leading to cross-polarized radia-
tion are p out of phase in Fig. 2, Band C. Aset of
eight antennas were thus created from the initial
four antennas, as shown in Fig. 2F. Full-wave sim-
ulations  confirm  that  the  amplitudes  of  the  cross-
polarizedradiationscatteredbythe eight antennas are
nearlyequal, withphases inp/4increments (Fig. 2G).
A  large  phase  coverage  (~300)  can  also  be
achieved by using arrays of straight antennas (fig.
S3). However, to obtain the same range of phase
shift  their scattering amplitudes  will  be  substan-
tially smaller than those of V-antennas (fig. S3).
As  a  consequence  of  its  double  resonances,  the
V-antenna instead allows one to design an array
with  phase  coverage  of  2p  and  equal,  yet  high,
scattering amplitudes for all of the array elements,
leading  to  anomalously  reflected  and  refracted
beams of substantially higher intensities.
Experiments   on   anomalous   reflection  and
refraction.  We  demonstrated  experimentally  the
generalized  laws   of   reflection  and  refraction
using  plasmonic  interfaces  constructed  by  peri-
odically arranging the eight constituent antennas
as explained in the caption of Fig. 2F. The spacing
between  the  antennas  should  be  subwavelength
so as to provide efficient scattering and to prevent
the occurrence of grating diffraction. However, it
should not be too small; otherwise, the strong near-
field  coupling  between  neighboring  antennas
would perturb the designed scattering amplitudes
and  phases.   A  representative  sample  with  the
densest packing of antennas, G = 11 mm, is shown
in  Fig.  3A,   where  G  is  the  lateral  period  of  the
antenna array. In the schematic of the experimen-
tal   setup  (Fig.   3B),   we  assume  that   the  cross-
polarized scattered light from the antennas on the
left  side  is  phase-delayed  as  compared  with  the
ones on the right. By substituting into Eq. 2  2p/G
for  dF/dx  and  the  refractive  indices  of  silicon
and  air  (n
Si
  and  1)  for  n
i
  and  n
t
,  we  obtain  the
angle of refraction for the cross-polarized beam
q
t,
 = arcsin[n
Si
sin(q
i
)    l
o
/G]
Figure 3C summarizes the experimental results
of the ordinary and the anomalous refraction for
six samples with different G at normal incidence.
The  incident   polarization  is  along  the  y  axis  in
Fig.  3A.  The  sample  with  the  smallest   G  corre-
sponds to the largest phase gradient and the most
Fig.   3.   (A)   Scanning  electron  microscope  (SEM)
image of a representative antenna array fabricated
on  a  silicon  wafer.  The  unit  cell  of  the  plasmonic
interface (yellow) comprises eight gold V-antennas
of  width  ~220  nm  and  thickness  ~50  nm,   and  it
repeats  with  a  periodicity  of   G  =  11  mm  in  the  x
direction and 1.5 mmin the y direction. (B) Schematic
experimental setup for y-polarized excitation (electric
field  normal   to  the  plane  of  incidence).   (C  and  D)
Measured  far-field  intensity  profiles  of  the  refracted
beams for y- and x-polarized excitations, respective-
ly. The refraction angle is counted from the normal
to the surface. The red and black curves are mea-
sured with and without a polarizer, respectively, for
six samples with different G. The polarizer is used to
select   the  anomalously  refracted  beams  that   are
cross-polarized  with  respect  to  the  excitation.  The
amplitude of the red curves is magnified by a factor
of   two  for   clarity.   The   gray   arrows   indicate   the
calculated angles of anomalous refraction according
to Eq. 6.
6
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   335
RESEARCH  ARTICLES
efficient  light  scattering  into  the  cross-polarized
beams.   We  observed  that  the  angles  of  anoma-
lous  refraction  agree  well   with  theoretical   pre-
dictions   of   Eq.   6  (Fig.   3C).   The   same   peak
positions   were  observed  for   normal   incidence,
with polarization along the x axis in Fig. 3A(Fig.
3D). To a good approximation, we expect that the
V-antennas  were  operating  independently  at  the
packing  density  used  in  experiments  (20).   The
purpose of using a large antenna array (~230  mm
by  230  mm)  is  solely  to  accommodate  the  size
of the plane-wavelike excitation (beam radius
~  100  mm).  The  periodic  antenna  arrangement
is used here for convenience but is not necessary
to  satisfy  the  generalized  laws  of  reflection  and
refraction.   It   is   only  necessary  that   the  phase
gradient is constant along the plasmonic interface
and that the scattering amplitudes of the antennas
are   all   equal.   The   phase   increments   between
nearest  neighbors  do  not  need  to  be  constant,  if
one  relaxes  the  unnecessary  constraint   of  equal
spacing between nearest antennas.
The  angles   of   refraction  and  reflection  are
shown  in  Fig.   4,   A  and  B,   respectively,   as   a
function  of   q
i
  for   both  the  silicon-air   interface
(black  curves  and  symbols)   and  the  plasmonic
interface  (red  curves  and  symbols)  (20).   In  the
range  of   q
i
  =  0  to  9,   the  plasmonic  interface
Fig.  4.  (A) Angle of refraction versus angle of incidence for the ordinary (black curve and triangles)
and  anomalous  refraction  (red  curve  and  dots)   for   the  sample  with  G  =  15  mm.   The  curves  are
theoretical   calculations   made  by  using  the  generalized  Snells   law  for   refraction  (Eq.   2),   and  the
symbols are experimental data extracted from refraction measurements as a function of the angle of
incidence  (20).   The  shaded  region  represents   negative  refraction  for  the  cross-polarized  light,   as
illustrated in the inset. The blue arrows indicate the modified critical angles for total internal reflection.
(B)  Angle  of  reflection  versus  angle  of  incidence  for  the  ordinary  (black  curve)  and  anomalous  (red
curve and dots) reflection for the sample with  G  = 15  mm. The top left inset is the zoom-in view. The
curves   are  theoretical   calculations   made  by  using  Eq.   4,   and  the  symbols   are  experimental   data
extracted  from  reflection  measurements  as  a  function  of  the  angle  of  incidence  (20).  The  shaded
region represents  negative reflection for the cross-polarized light, as illustrated in the bottom right
inset. The blue arrow indicates the critical angle of incidence above which the anomalously reflected
beam becomes evanescent. Experiments with lasers emitting at different wavelengths show that the
plasmonic interfaces are broadband, anomalously reflecting and refracting light from  l   5  mm to  l  
10  mm.
Fig.  5.  (A) SEM image of a plasmonic interface that
creates   an   optical   vortex.   The   plasmonic   pattern
consists   of   eight   regions,   each   occupied   by   one
constituent antenna of the eight-element set of Fig.
2F.  The  antennas  are  arranged  so  as  to  generate  a
phase shift that varies azimuthally from 0 to 2p, thus
producing a helicoidal scattered wavefront. (B) Zoom-in
view of the center part of (A). (C and D) Respectively,
measured and calculated far-field intensity distributions
of  an  optical  vortex  with  topological  charge  one.  The
constant  background  in  (C)  is  due  to  the  thermal  ra-
diation.   (E  and  F)  Respectively,   measured  and  calcu-
lated spiral patterns created by the interference of the
vortex beam and a co-propagating Gaussian beam. (G
and H) Respectively, measured and calculated interfer-
ence  patterns  with  a  dislocated  fringe  created  by  the
interference of the vortex beam and a Gaussian beam
when the two are tilted with respect to each other. The
circular border of the interference pattern in (G) arises
from the finite aperture of the beam splitter used to
combine the vortex and the Gaussian beams (20). The
size of (C) and (D) is 60 mmby 60 mm, and that of (E)
to (H) is 30 mm by 30 mm.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 336
RESEARCH  ARTICLES
exhibits  negative  refraction  and  reflection  for
the cross-polarized scattered light (schematics are
shown in the bottom right insets of Fig. 4, A and
B). The critical angle for total internal reflection
is modified to ~8 and +27 (Fig. 4A, blue ar-
rows)  for  the  plasmonic  interface  in  accordance
with Eq. 3, compared with T17 for the silicon-air
interface; the anomalous reflection does not exist
beyond  q
i
 =  57 (Fig. 4B, blue arrow).
At  normal  incidence,  the  ratio  of  intensity  R
between the anomalously and ordinarily refracted
beams  is  ~0.32  for  the  sample  with  G  =  15  mm
(Fig. 3C).  R rises for increasing antenna packing
densities (Fig. 3, C and D) and increasing angles
of   incidence  [up  to  R     0.97  at   q
i
  =  14  (fig.
S1B)]. Because of the experimental configuration,
we are not able to determine the ratio of intensity
between  the  reflected  beams  (20),  but  we  expect
comparable values.
Vortex beams created by plasmonic interfaces.
To  demonstrate  the  versatility  of  the  concept  of
interfacial  phase  discontinuities,  we  fabricated  a
plasmonic interface that is able to create a vortex
beam (21,  22) upon illumination by normally in-
cident linearly polarized light. Avortex beamhas
a helicoidal (or corkscrew-shaped) equal-phase
wavefront.   Specifically,   the   beam  has   an   azi-
muthal phase dependence exp(il) and carries an
orbital angular momentum of  L  l per photon
(23). Here, the topological charge  l is an integer,
indicating the number of twists of the wavefront
within one wavelength;  is the azimuthal angle
with  respect   to  the  beam  axis;   and     is   the
reduced Planck constant. These peculiar states
of light are commonly generated by using a spiral
phase  plate  (24)   or   a  computer-generated  holo-
gram (25) and can be used to rotate particles (26)
or to encode information in optical communica-
tion systems (27).
The plasmonic interface was created by arrang-
ing  the  eight   constituent   antennas  as  shown  in
Fig. 5, Aand B. The interface introduces a spiral-
like phase shift with respect to the planar wave-
front of the incident light, creating a vortex beam
with  l  =  1.  The  vortex  beam  has  an  annular  in-
tensity distribution in the cross section, as viewed
in  a  mid-infrared  camera  (Fig.  5C);  the  dark  re-
gion  at  the  center  corresponds  to  a  phase  singu-
larity  (22).  The  spiral  wavefront  of  the  vortex
beam  can  be  revealed  by  interfering  the  beam
with  a  co-propagating  Gaussian  beam  (25),  pro-
ducing a spiral interference pattern (Fig. 5E). The
latter rotates when the path length of the Gaussian
beam  was  changed  continuously  relative  to  that
of the vortex beam (movie S1). Alternatively, the
topological   charge  l   =  1  can  be  identified  by  a
dislocated interference fringe when the vortex and
Gaussian beams interfere with a small angle (Fig.
5G)  (25).  The  annular  intensity  distribution  and
the interference patterns were well reproduced in
simulations  (Fig.   5,   D,   F,   and  H)  by  using  the
calculated amplitude and phase responses of the
V-antennas (Fig. 2, D and E).
Concluding  remarks.   Our  plasmonic  inter-
faces,  consisting  of  an  array  of  V-antennas,  im-
part  abrupt  phase  shifts  in  the  optical  path,  thus
providing great  flexibility in molding of the op-
tical wavefront. This breaks the constraint of stan-
dard optical  components,  which rely on gradual
phase  accumulation  along  the  optical   path  to
change  the  wavefront   of  propagating  light.   We
have derived and experimentally confirmed gen-
eralized reflection and refraction laws and studied
a  series  of   intriguing  anomalous  reflection  and
refraction  phenomena   that   descend  from  the
latter: arbitrary reflection and refraction angles
that   depend   on   the   phase   gradient   along   the
interface,   two  different   critical   angles   for   total
internal   reflection   that   depend   on  the   relative
direction of the incident light with respect to the
phase gradient, and critical angle for the reflected
beam  to  be   evanescent.   We  have  also  used  a
plasmonic  interface  to  generate  optical   vortices
that have a helicoidal wavefront and carry orbit-
al   angular   momentum,   thus   demonstrating  the
power  of  phase  discontinuities  as  a  design  tool
of complex beams. The design strategies presented
in  this  article  allow  one  to  tailor   in  an  almost
arbitrary   way   the   phase   and   amplitude   of   an
optical wavefront, which should have major im-
plications for transformation optics and integrated
optics.   We  expect   that   a  variety  of  novel   planar
optical components such as phased antenna arrays
in  the  optical   domain,   planar  lenses,   polarization
converters,   perfect   absorbers,   and   spatial   phase
modulators  will  emerge  from  this  approach.
Antenna   arrays   in   the   microwave   and
millimeter-wave  regions  have  been  used  for   the
shaping  of  reflected  and  transmitted  beams  in
the  so-called  reflectarrays  and  transmitarrays
(2831). These typically consist of a double-layer
structure comprising a planar array of antennas
and a ground plane (in the case of reflectarrays)
or  another  array  (in  the  case  of  transmitarrays),
separated  by  a  dielectric  spacer   of  finite  thick-
ness. Reflectarrays and transmitarrays cannot be
treated  as  a  single  interface  for  which  one  can
write  down  the  generalized  laws   because  they
rely  on  both  antenna  resonances  and  the  propa-
gation  of   waves   in  the   spacer   to  achieve   the
desired  phase  control.  The  generalization  of  the
laws  of   reflection  and  refraction  we  present   is
made possible by the deeply subwavelength thick-
ness of our optical antenna arrays and their asso-
ciated abrupt phase changes, with no contribution
from propagation effects. These generalized laws
apply  to the whole optical  spectrum  for suitable
designer   interfaces  and  can  be  a  guide  for   the
design of new photonic devices.
References  and  Notes
1.   J.  B.  Pendry,  D.  Schurig,  D.  R.  Smith,  Science  312,  1780
(2006).
2.   U.   Leonhardt,   Science  312,  1777  (2006).
3.   W.  Cai,  V.  Shalaev,  Optical  Metamaterials:  Fundamentals
and  Applications  (Springer,   New  York,   2009).
4.   N. Engheta, R. W. Ziolkowski,  Metamaterials: Physics  and
Engineering  Explorations  (Wiley-IEEE  Press,   New  York,
2006).
5.   I.   I.   Smolyaninov,   E.  E.   Narimanov,   Phys.   Rev.   Lett.   105,
067402  (2010).
6.   S. D. Brorson, H. A. Haus, J. Opt. Soc. Am. B 5, 247 (1988).
7.   R.   P.   Feynman,   A.   R.   Hibbs,   Quantum  Mechanics  and
Path  Integrals  (McGraw-Hill,   New  York,   1965).
8.   E.   Hecht,   Optics  (Addison  Wesley,   Boston,   ed.   3,
1997).
9.   H. T. Miyazaki, Y. Kurokawa, Appl. Phys. Lett. 89, 211126
(2006).
10.   D.   Fattal,   J.   Li,   Z.   Peng,   M.   Fiorentino,   R.   G.  Beausoleil,
Nat.   Photonics  4,   466  (2010).
11.   J.   A.   Fan  et  al.,   Science  328,  1135  (2010).
12.   B.   Lukyanchuk  et  al.,   Nat.   Mater.   9,  707  (2010).
13.   R.   D.   Grober,   R.   J.   Schoelkopf,   D.   E.  Prober,   Appl.   Phys.
Lett.   70,   1354  (1997).
14.   L.   Novotny,   N.   van  Hulst,   Nat.   Photonics  5,  83
(2011).
15.   Q.   Xu  et  al.,   Nano  Lett.   7,  2800  (2007).
16.   M.   Sukharev,   J.   Sung,   K.   G.   Spears,   T.   Seideman,
Phys.   Rev.   B  76,  184302  (2007).
17.   P.   Biagioni,   J.   S.   Huang,   L.   Du,  M.   Finazzi,  B.   Hecht,
Phys.   Rev.   Lett.   102,   256801  (2009).
18.   S.   Liu  et  al.,   Opt.   Lett.   34,  1255  (2009).
19.   J.   Ginn,   D.   Shelton,   P.   Krenz,   B.   Lail,   G.   Boreman,
Opt.   Express  18,   4557  (2010).
20.   Materials  and  methods  are  available  as  supporting
material   on  Science  Online.
21.   J.   F.   Nye,   M.   V.   Berry,   Proc.   R.   Soc.   London  A  Math.
Phys.   Sci.   336,   165  (1974).
22.   M.   Padgett,   J.   Courtial,   L.   Allen,   Phys.   Today  57,  35
(2004).
23.   L.   Allen,   M.   W.   Beijersbergen,  R.   J.   C.   Spreeuw,
J.   P.   Woerdman,  Phys.   Rev.   A  45,  8185  (1992).
24.   M.   W.   Beijersbergen,  R.   P.   C.   Coerwinkel,   M.   Kristensen,
J.   P.   Woerdman,  Opt.   Commun.  112,   321  (1994).
25.   N.   R.   Heckenberg,   R.   McDuff,  C.   P.   Smith,   A.   G.  White,
Opt.   Lett.   17,   221  (1992).
26.   H.  He,  M.  E.  J.  Friese,  N.  R.  Heckenberg,   H.  Rubinsztein-
Dunlop,   Phys.   Rev.   Lett.   75,   826  (1995).
27.   G.   Gibson  et  al.,   Opt.  Express  12,  5448  (2004).
28.   D.   M.   Pozar,   S.  D.   Targonski,  H.   D.   Syrigos,   IEEE  Trans.
Antenn.   Propag.  45,  287  (1997).
29.   J.   A.   Encinar,   IEEE  Trans.   Antenn.   Propag.  49,  1403
(2001).
30.   C.   G.  M.   Ryan  et  al.,   IEEE  Trans.   Antenn.   Propag.  58,
1486  (2010).
31.   P.   Padilla,   A.   Muoz-Acevedo,   M.   Sierra-Castaer,
M.   Sierra-Prez,   IEEE  Trans.   Antenn.   Propag.  58,   2571
(2010).
Acknowledgments:  The  authors  acknowledge  helpful
discussion  with  J.   Lin,   R.   Blanchard,   and  A.   Belyanin.
The  authors  acknowledge  support  from  the  National
Science  Foundation  (NSF),   Harvard  Nanoscale  Science
and  Engineering  Center  (NSEC)  under  contract
NSF/PHY  06-46094,  and  the  Center  for  Nanoscale
Systems  (CNS)  at  Harvard  University.   This  work  was
supported  in  part  by  the  Defense  Advanced  Research
Projects  Agency  (DARPA)  N/MEMS  S&T  Fundamentals
program  under  grant  N66001-10-1-4008  issued  by  the
Space  and  Naval   Warfare  Systems  Center  Pacific
(SPAWAR).   Z.G.   acknowledges  funding  from  the
European  Communities  Seventh  Framework  Programme
(FP7/2007-2013)  under  grant  agreement  PIOF-GA-
2009-235860.   M.A.K.   is  supported  by  NSF  through  a
Graduate  Research  Fellowship.   Harvard  CNS  is  a
member  of  the  National   Nanotechnology  Infrastructure
Network.   The  Lumerical   (Vancouver,   BC,  Canada)
FDTD  simulations  in  this  Research  Article  were  run
on  the  Odyssey  cluster  supported  by  the  Harvard
Faculty  of  Arts  and  Sciences  Sciences  Division  Research
Computing  Group.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1210713/DC1
Materials  and  Methods
SOM  Text
Figs.   S1  to  S6
References  (3239)
Movie  S1
5  July  2011;   accepted  19  August  2011
Published  online  1  September  2011;
10.1126/science.1210713
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   337
RESEARCH  ARTICLES
Detection  of   the  Water  Reservoir  in  a
Forming  Planetary  System
Michiel  R.  Hogerheijde,
1
*  Edwin  A.  Bergin,
2
Christian  Brinch,
1
L.  Ilsedore  Cleeves,
2
Jeffrey  K.  J.  Fogel,
2
Geoffrey  A.  Blake,
3
Carsten  Dominik,
4
Dariusz  C.  Lis,
5
Gary  Melnick,
6
David  Neufeld,
7
Olja  Pani,
8
John  C.  Pearson,
9
Lars  Kristensen,
1
Umut  A.  Yldz,
1
Ewine  F.  van  Dishoeck
1,10
Icy  bodies  may  have  delivered  the  oceans  to  the  early  Earth,  yet  little  is  known  about  water  in
the  ice-dominated  regions  of  extrasolar  planet-forming  disks.  The  Heterodyne  Instrument  for  the
Far-Infrared  on  board  the  Herschel  Space  Observatory  has  detected  emission  lines  from  both  spin
isomers  of  cold  water  vapor  from  the  disk  around  the  young  star  TW  Hydrae.  This  water  vapor
likely  originates  from  ice-coated  solids  near  the  disk  surface,  hinting  at  a  water  ice  reservoir
equivalent  to  several  thousand  Earth  oceans  in  mass.  The  waters  ortho-to-para  ratio  falls  well
below  that  of  solar  system  comets,  suggesting  that  comets  contain  heterogeneous  ice  mixtures
collected  across  the  entire  solar  nebula  during  the  early  stages  of  planetary  birth.
W
ater  in  the  solar  nebula  is  thought   to
have been frozen out onto dust grains
outside   3  astronomical   units  (AU)
(1, 2). Stored in icy bodies, this water provided a
reservoir   for   impact   delivery  of   oceans   to  the
Earth (3). In planet-forming disks, water vapor is
thought to be abundant only in the hot (>250 K)
inner regions, where ice sublimates and gas-phase
chemistry locks up all oxygen in H
2
O. Emission
from hot (>250 K) water has been detected from
several   disks  around  young  stars  (4,   5).   In  the
cold (20 K) outer disk, water vapor freezes out,
evidenced  by  spectral  features  of  water  ice  in  a
few  disks  (6,   7).   However,   (inter)stellar  ultravi-
olet   radiation  penetrating  the  upper   disk  layers
desorbs  a  small  fraction  of  water  ice  molecules
back into the gas phase (8), suggesting that cold
(<100 K) water vapor exists throughout the radial
extent   of   the  disk.   The  detection  of   this  water
vapor would signal the presence of a hidden ice
reservoir.
We report detection of ground-state rotation-
al emission lines of both spin isomers of water
(J
KAKC
1
10
-1
01
  from  ortho-H
2
O  and 1
11
-0
00
  from
para-H
2
O)  from  the  disk  around  the  premain-
sequence  star  TW  Hydrae  (TW  Hya)  using  the
Heterodyne Instrument for the Far-Infrared (HIFI)
spectrometer   (9)   on  board  the  Herschel   Space
Observatory (10) (Fig. 1) (11,  12). TW Hya is
a  0.6  M
in gas (1416).
The  velocity  widths  of   the  H
2
O  lines  (0.96  to
1.17 kms
1
) (table S1) exceed by 40%those of
cold CO (14). These correspond to CO emission
fromthe full 196-AU-radius rotating disk inclined
at 7 with only little (<65 ms
1
) turbulence (17).
The wider H
2
O lines suggest that the water emis-
sion extends to 115 AU, where the gas orbits
the   star   at   higher   velocities   compared  with
196 AU.
To quantify the amount of water vapor traced
by the detected lines, we performed detailed sim-
ulations   of   the   water   chemistry   and   line   for-
mation  using  a   realistic   disk  model   matching
previous   observations   (12,   18).   We   adopted  a
conservatively low  dust  mass of 1.9  10
4
M
. We explored
the effects of much lower gas-to-dust ratios. We
followed the penetration of the stellar ultraviolet
and  x-ray  radiation  into  the  disk;  calculated  the
resulting  photodesorption  of  water  and  ensuing
gas-phase chemistry, including photodissociation;
and  solved  the  statistical-equilibrium  excitation
and line formation. The balance of photodesorption
of water ice and photodissociation of water vapor
results in an equilibrium column of water H
2
O
vapor  throughout  the  disk  (Fig.  2).  Consistent
with other studies (19), we find a layer of max-
imum water vapor abundance of 0.5  10
7
to
2  10
7
relative to H
2
at an intermediate height in
the   disk.   Above   this   layer,   water   is   photodis-
sociated;   below  it,   little  photodesorption  occurs
and water is frozen out, with an ice abundance, set
by available oxygen, of 10
4
relative to H
2
.
In  our   model,   the   100-   to  196-AU  region
dominates  the line  emission,  which exceeds  ob-
servations in strength by factors of 5.3  T  0.2 for
H
2
O  1
10
-1
01
  and  3.3  T  0.2  for  H
2
O  1
11
-0
00
.   A
lower   gas  mass  does  not   decrease  the  line  in-
tensities,   if  we  assume  that   the  water  ice,   from
1
Leiden Observatory, Leiden University, Post Office Box 9513,
2300 RA Leiden, Netherlands.
2
Department of Astronomy, Uni-
versity of Michigan, Ann Arbor, MI 48109, USA.
  3
Division of
Geological and Planetary Sciences, California Institute of Tech-
nology,   Pasadena,   CA  91125,   USA.
  4
Astronomical   Institute
Anton  Pannekoek,   University  of   Amsterdam,   1098  XH  Am-
sterdam, Netherlands.
  5
Division of Physics, Mathematics, and
Astronomy,   California  Institute  of   Technology,   Pasadena,   CA
91125,   USA.
  6
Harvard-Smithsonian  Center   for   Astrophysics,
Cambridge, MA 02138, USA.
  7
Department of Physics and As-
tronomy,   Johns   Hopkins   University,   Baltimore,   MD  21218,
USA.
  8
European Southern Observatory, 85748 Garching, Ger-
many.
  9
Jet Propulsion Laboratory, California Institute of Tech-
nology,  Pasadena,  CA  91109,   USA.
  10
Max-Planck-Institut  fr
Extraterrestrische Physik, 85748 Garching, Germany.
*To   whom  correspondence   should   be   addressed.   E-mail:
michiel@strw.leidenuniv.nl
Fig.   1.   Spectra   of   para-H
2
O
1
11
-0
00
 (A) and ortho-H
2
O 1
10
-
1
01
  (B)   obtained  with  HIFI   on
the Herschel Space Observatory
toward  the  protoplanetary  disk
around TWHya after subtraction
of the continuum emission. The
vertical   dotted  lines  show  the
systems velocity of +2.8 km s
1
relative  to  the  Suns   local   en-
vironment   (local   standard   of
rest).
REPORTS
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 338
which  the  water  vapor  derives,   formed  early  in
the  disks  evolution,   before  substantial   gas  loss
occurred, and remains frozen on grains. The most
plausible explanation involves a difference in the
relative  location  of  small,  bare  grains  regulating
the ultraviolet radiative transport and larger, ice-
carrying grains. Differential settling of large grains
relative  to  small   grains  moves  much  of  the  ice
reservoir   below  the  reach  of   the  ultraviolet   ra-
diation, resulting in less water vapor and weaker
lines. Our model matches the observations if only
12%  of  the  original   ice  content   remains  above
this   line  (20).   A  radially  increasing  degree  of
settling of icy grains explains the observed H
2
O
line widths.
The   detected   water   vapor,   resulting   from
photodesorption,   implies  an  ice  reservoir  in  the
giant  planet  formation  zone  and  beyond.  In  our
simulations,   the  7.3    10
24
g  of  detected  water
vapor   (equivalent   to  0.005  times   the   mass   of
Earths  oceans)  originate  from  a  total   ice  reser-
voir of 9  10
27
g (or several thousands of Earths
oceans) throughout the disk. The size of this res-
ervoir  is  tied  to  the  dust   mass  contained  in  the
disk,   for  which  we  adopt   a  conservatively  low
value. Although the ice reservoir is only observed
indirectly,   no  known  mechanism  can  remove  it
from the regions probed by Herschel. Any small-
er   ice   reservoir   implies   the   corresponding  ab-
sence of elemental oxygen that efficiently reforms
water ice on the grains.
The  detection  of  both  spin  isomers  of  water
vapor  allows  its  ortho-to-para  ratio  (OPR)  to  be
derived, because our simulations indicate that the
lines  are  optically  thin.  An  OPR  of  0.77  T  0.07
matches   our   observations   (12).   This   value   is
much  lower  than  the  OPR  range  of  2  to  3  ob-
served  for  solar  system  comets  (21).   It  is  com-
mon  practice  to  associate  the  OPR  with  a  spin
temperature   T
spin
  at   which  a  Boltzmann  distri-
bution reproduces the ratio of spin isomers. Our
derived OPR corresponds to T
spin
 = 13.5  T 0.5 K,
whereas the range for solar system comets yields
a  T
spin
 of   >20 K.
Radiative conversion between spin isomers is
not allowed in the gas phase, preserving the OPR
for long time scales. Gas-phase formation of wa-
ter  occurs  through  exothermic  reactions  leading
to an OPR of 3. On grains, water forms and sur-
vives  at  low  temperatures,  and  it  is  tempting  to
equate T
spin
with the grain temperature. However,
the  energetics  of  water  formation  and  ortho-to-
para  exchange  on  grains  are  poorly  understood
(22),   and  the  water   OPR  may  be  changed  by
photodesorption. This process starts by dissociat-
ing water to H and OH in the ice and continues
with  the  energetic  H  kicking  out  a  neighboring
H
2
O molecule from the ice matrix or with the H
and OHrecombining in the ice to formH
2
Owith
sufficient  internal  energy  to  sublimate  (23).  The
latter  route  drives the  OPR  to  at  least  unity,  im-
plying an even lower original ice OPR, to yield a
resulting  OPR  of   0.77.   Cometary  volatiles   are
released  through  thermal   sublimation,   and  their
measured OPRs are interpreted to reflect the OPR
of  their  ice  constituents.  Equating  T
spin
  with  the
physical   temperature  of  the  grain  on  which  the
ice formed is supported by the similarity of mea-
sured  T
spin
 of NH
3
 and H
2
O in several individual
solar system comets (24).
Solar   system  comets  consist   of   a  heteroge-
neous  mixture  of  ices  and  solids,   likely  assem-
bled in the giant planet formation zone by mixing
local  material  with  material  that  drifted  in  from
larger  radii   (25).   Our  water  vapor  observations
probe cold, ice-coated precometary grains resid-
ing beyond >50 AU, representing the bulk of the
latter  material.   The  presence  in  comets  of  crys-
talline silicates, requiring formation temperatures
>800 K(26), together with COand H
2
Oices that
condense at 20 to 100 K, argues for transport of
hot   material   from  near  the  star  to  the  icy  outer
regions  of   the  solar   nebula  (27).   Provided  that
spin temperatures reflect formation histories, the
different   T
spin
  inferred  for  the  water  ice  in  TW
Hya  (<13  K)  and  solar  system  comets  (>20  K)
indicates a similar mixing of volatiles throughout
the entire solar nebula, blending water formed at
>50 K and an OPR of 3 with water formed at 10
to 20 K and an OPR < 1 probed by our observa-
tions. In this case, the range of T
spin
 values of the
cometary inventory reflects the stochastic nature
of transport and mixing.
Our Herschel detection of cold water vapor in
the outer disk of TW Hya demonstrates the pres-
ence  of  a  considerable  reservoir  of  water  ice  in
this protoplanetary disk, sufficient to formseveral
thousand Earth oceans worth of icy bodies. Our
observations only directly trace the tip of the ice-
berg of 0.005 Earth oceans in the form of water
vapor.
References  and  Notes
1.   One astronomical unit (AU) is the mean distance between
Earth  and  the  Sun  of  1.49598    10
11
m.
2.   C.   Hayashi,   Prog.   Theor.   Phys.   70  (suppl.),  35
(1981).
3.   T.   Matsui,   Y.   Abe,   Nature  322,   526  (1986).
4.   K.   M.   Pontoppidan,  C.   Salyk,   G.   A.   Blake,  H.   U.   Kufl,
Astrophys.   J.   722,   L173  (2010).
5.   J.   S.  Carr,   J.   R.   Najita,  Astrophys.   J.  733,  102
(2011).
6.   H.   Terada  et  al.,   Astrophys.   J.  667,  303  (2007).
7.   M.   Honda  et  al.,   Astrophys.   J.   690,  L110
(2009).
8.   C.   Dominik,   C.  Ceccarelli,  D.   Hollenbach,   M.   Kaufman,
Astrophys.   J.   635,   L85  (2005).
9.   T.   de  Graauw  et  al.,   Astron.   Astrophys.   518,  L6
(2010).
10.   G.   L.   Pilbratt  et  al.,   Astron.   Astrophys.   518,   L1
(2010).
11.   Water  in  Earths  atmosphere  obstructs  ground-based
detection  of  cold  water  vapor  in  planet-forming  disks.
Although  Herschel   cannot  spatially  resolve  even  the
closest  disk  in  water  ground-state  emission  lines,  HIFI
spectrally  resolves  the  H
2
O  line  profiles.   Comparison
with  previous  spectrally  and  spatially  resolved
observations  of  CO  confirms  the  disk  origin  of  the
H
2
O  lines.
12.   Materials  and  methods  are  available  as  supporting
material   on  Science  Online.
13.   R.   A.   Webb  et  al.,   Astrophys.   J.   512,   L63  (1999).
14.   J. H. Kastner, B. Zuckerman, D. A. Weintraub, T. Forveille,
Science  277,  67  (1997).
15.   N.   Calvet  et  al.,   Astrophys.   J.   568,  1008  (2002).
16.   U.  Gorti,  D.  Hollenbach,  J.  Najita,  I.  Pascucci,  Astrophys.  J.
735,  90  (2011).
17.   A.   M.   Hughes,   D.   J.   Wilner,   S.  M.   Andrews,   C.   Qi,
M.   R.   Hogerheijde,   Astrophys.   J.  727,  85  (2011).
18.   W.   Thi   et  al.,   Astron.   Astrophys.   518,   L125  (2010).
19.   P.   Woitke,   W.   Thi,  I.   Kamp,   M.  R.   Hogerheijde,
Astron.   Astrophys.   501,  L5  (2009).
20.   R.   Meijerink,   K.   M.   Pontoppidan,   G.  A.   Blake,
D.  R.  Poelman,  C. P.  Dullemond,  Astrophys.  J. 704,  1471
(2009).
A
C   D
B
Fig. 2. Adopted model for the TWHya protoplanetary disk. (A) H
2
number density, (B) dust temperature,
(C) the number density of water vapor molecules and contours of volume-averaged water ice abundance
decreasing from white to black as 2  10
4
, 2  10
5
, 2  10
6
, 2  10
7
, and 2  10
8
, relative to H
2
,
and (D) one quadrant of the resulting water emission line intensity fromthe near face-on disk, in arbitrary
units. In (A) and (B), the blue contour delineates the layer of maximum water vapor abundance.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   339
REPORTS
21.   B.  P.   Bonev  et  al.,   Astrophys.   J.   661,   L97
(2007).
22.   H.-H.   Limbach  et  al.,   ChemPhysChem  7,  551
(2006).
23.   S.  Andersson,  E.  F.  van  Dishoeck, Astron.  Astrophys.  491,
907  (2008).
24.   Y.   Shinnaka  et  al.,   Astrophys.   J.  729,  81  (2011).
25.   S.  J.   Weidenschilling,   Mon.   Not.  R.   Astron.   Soc.   180,  57
(1977).
26.   S.  A.   Sandford  et  al.,   Science  314,   1720
(2006).
27.   D.   H.   Wooden,  Space  Sci.   Rev.   138,  75
(2008).
Acknowledgments:   Herschel   is  a  European  Space  Agency
space  observatory  with  science  instruments  provided  by
European-led  principal   investigator  consortia  and  with
important  participation  from  NASA.   This  work  was
partially  supported  by  Nederlandse  Organisatie  voor
Wetenschappelijk  Onderzoek  grant  639.042.404,   NSF
grant  0707777,   and,   as  part  of  the  NASA  Herschel   HIFI
guaranteed  time  program,   NASA.   The  data  presented
here  are  archived  at  the  Herschel   Science  Archive,
http://archives.esac.esa.int/hda/ui,   under  OBSID
1342198337  and  1342201585.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/338/DC1
Materials  and  Methods
Table  S1
References  (2839)
25  May  2011;   accepted  20  September  2011
10.1126/science.1208931
Supramolecular  Linear  Heterojunction
Composed  of   Graphite-Like
Semiconducting  Nanotubular  Segments
Wei Zhang,
1,2
Wusong Jin,
3
Takanori Fukushima,
1,4
* Akinori Saeki,
5
Shu Seki,
5
Takuzo Aida
1,2
*
One-dimensionally connected organic nanostructures with dissimilar semiconducting properties are
expected to provide a reliable platform in understanding the behaviors of photocarriers, which are
important for the development of efficient photon-to-electrical energy conversion systems. Although
bottom-up supramolecular approaches are considered promising for the realization of such nanoscale
heterojunctions, the dynamic nature of molecular assembly is problematic. We report a
semiconducting nanoscale organic heterojunction, demonstrated by stepwise nanotubular
coassembly of two strategically designed molecular graphenes. The dissimilar nanotubular segments,
thus connected noncovalently, were electronically communicable with one another over the
heterojunction interface and displayed characteristic excitation energy transfer and charge transport
properties not present in a mixture of the corresponding homotropically assembled nanotubes.
H
eterojunctions,  occurring  between  two
dissimilar semiconducting materials, are
expected  to  provide  peculiar   electronic
properties  that  are  hard  to  realize  by  homojunc-
tions.   Heterojunctions   of   varying  dimensions
are readily fabricated from inorganic semicon-
ductors and lead to many applications, including
solid-state  lasers,  diodes,  solar  cells,  and  tran-
sistors (16). Organic heterojunctions are of im-
portance in the development of organic thin-film
solar cells (7,   8). However, most that have been
studied are  so-called bulk heterojunctions,  which
are formed only coincidentally fromdonor/acceptor
mixtures upon phase separation (912). Although
bottom-up  supramolecular   approaches  (13,   14)
are a potent tool for the formation of organic het-
erojunctions,  such  studies  have  just  started  with
molecularly  engineered  donor/acceptor   couples
(1519). From a fundamental viewpoint, one chal-
lenge would be to tailor a linear organic hetero-
junction   at   the   nanoscale   by   joining   together
dissimilar  semiconducting  one-dimensional  mo-
lecular objects, because one has to overcome the
essential   problem  arising   from  the   dynamic
nature  of  molecular  assembly  (13,   14,   2024).
We reported that a Gemini-shaped hexa-peri-
hexabenzocoronene (HBC) derivative, bearing
two triethylene glycol-appended phenyl groups
on  one  side  of  the  HBC  core  and  dodecyl  side
chains  on  the  other,  self-assembles  into  a  semi-
conducting nanotube with inner and outer diam-
eters  of  14  and  20  nm,  respectively  (25,   26).  A
recent   structural   analysis  using  a  synchrotron
x-ray diffraction technique revealed that the nano-
tube is  composed of a graphite-like bilayer wall
consisting of helically twisted columnar arrays
of   p-stacked  HBC  units  (26).   For  the  realiza-
tion of a nanotubular heterojunction using this
self-assembling motif, essential requisites are (i)
the  formation  of  a  morphologically  stabilized
seed  nanotube  and  (ii)  the  design  of  a  second
graphene  monomer  capable  of  tubularly  assem-
bling  from  the  extremely  thin  facets  of  the  seed
nanotube  termini.   Further   issues  include  how  to
cope  with  a  high  dispersibility  of  the  seed  nano-
tube  and  a  solubility  of  the  second  monomer
under  assembling  conditions.
A  keen  examination,  taking  into  account  all
the  above  requisites,  led  us  to  HBC  derivatives
1  and  2  (27)  as  the  monomers  for  the  seed  and
second  nanotubular   segment,   respectively  (Fig.
1). HBC  1 carries two bipyridine (bpy) units, in
order  for  the  resulting  seed  nanotube  (Fig.   1A)
to  be  morphologically  stabilized  by  wrapping
with  a  metal-coordination  network  (Fig.   1  B)
(28). The charged surface of the resultant seed
also  merits  its  homogeneous  dispersion  by  an
electrostatic repulsion (29). On the other hand,
HBC  2 bears four electron-withdrawing fluorine
substituents,   so  it   can  adhere  electronically  to
the  seed  termini  and  self-assemble  selectively
from their nanotubular facets. When these HBC
molecules   coassemble   stepwise   (Fig.   1C),   the
resultant  connecting  segments  are  electronically
dissimilar  to  one  another  (Fig.  1D).
As a typical example of the preparation of the
seed  nanotube  (NT
1Cu
,   Fig.   1B),   a  5-ml   glass
vial containing a tetrahydrofuran (THF) solution
(2.0 ml) of HBC  1 (0.5 mg, 1.5  10
4
M) was
placed in a 50-ml glass vial containing 10 ml of
methanol (MeOH) and allowed to stand at 25C,
whereupon a yellow suspension gradually formed.
Absorption spectroscopy of the suspension after
a  24-hour  incubation  (fig.  S1,  A  and  B,  broken
curve)   showed  red-shifted  absorption  bands   at
426  and  459  nm  characteristic  of   J-aggregated
HBCs  (25,   26).   Scanning  electron  microscopy
(SEM,   fig.   S2A)  and  transmission  electron  mi-
croscopy (TEM, fig. S2B) of an air-dried sample
of   the  suspension  allowed  for   visualizing  nano-
tubes  (NT
1
)  with  a  uniform  diameter  of  20  nm,
although  they  were  heavily  bundled  (Fig.   1A)
just  like  other  HBC  nanotubes  (25,   26).  We  in-
vestigated the metal-coordination capability of
NT
1
 by using Cu
2+
, because bpy is known to bind
to Cu
2+
, affording a bpy
2
Cu
2+
complex. As soon
as  a  MeOH  solution  (1.0  ml)  of  copper(II)  tri-
fluoromethanesulfonate [Cu(OTf )
2
, 0.5 mg, 1.5 
10
6
mol;  5.0  equivalents  to  HBC  1]  was  added,
the  suspension  containing  bundled  NT
1
  became
clear, suggesting that Cu
2+
ions are bound to the
surface  bpy  groups  (Fig.   1,   A  to  B)  and  make
the nanotubes (NT
1Cu
) electrostatically repulsive
from  one  another  (29).  When  an  air-dried  sam-
ple of  NT
1Cu
, isolated by filtration and washed
with MeOH to remove free Cu(OTf )
2
, was sub-
jected to SEM, highly dispersed nanotubes were
observed  (fig.   S3A).   Complete  coordination  of
Cu
2+
with bpy-appended HBC  1 was confirmed
by matrix-assisted laser desorption ionization time-
of-flight  (MALDI-TOF)  mass  spectrometry  of
isolated  NT
1Cu
  (fig.   S4);   no  peaks  attributable
to  metal-free  1  were  detected,   but   those  assign-
able to  1Cu, dissociated from  NT
1Cu
, were. The
metal   coordination  of   NT
1
  did  not   give  rise  to
any shift of the  J-aggregate absorption bands (426
and  459  nm;  fig.  S1B,  solid  curve).  Hence,  the
p-stacking  geometry  of  the  HBC  units  is  intact
1
Functional   Soft   Matter   Research  Group,   RIKEN  Advanced
Science  Institute,  2-1 Hirosawa,  Wako, Saitama  351-0198,
Japan.
  2
Department of Chemistry and Biotechnology, School of
Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku,
Tokyo 113-8656, Japan.
  3
College of Chemistry, Chemical Engi-
neering  and  Biotechnology,   Donghua  University,   2999  North
Renmin Road, Songjiang, Shanghai 201620, Peoples Republic
of   China.
  4
Chemical   Resources   Laboratory,   Tokyo  Institute  of
Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503,
Japan.
  5
Graduate School of Engineering, Osaka University, 2-1
Yamadaoka,  Suita,  Osaka  565-0871,  Japan.
*To   whom  correspondence   should   be   addressed.   E-mail:
fukushima@riken.jp  (T.F.);  aida@macro.t.u-tokyo.ac.jp  (T.A.)
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 340
REPORTS
even with the formation of a metal-coordination
network  on  the  nanotube  surface.
We investigated whether HBC  2 alone has the
ability  to  form  a  nanotubular  assembly.   On  the
basis of a computational study using density func-
tional theory (DFT), the core of HBC  2 with four
fluorine  substituents  most  likely  adopts  a  slightly
twisted,   concave  structure  (fig.   S5).   Probably  be-
cause  of  this  skeletal   distortion,   HBC  2  was  un-
able to assemble into nanotubes under a variety of
conditions used previously (16,  18,  25,  26,  28,  29).
However,  we  eventually  found  that,  in  acetone,
2  self-assembles  into  tubules.   This  observation
was  unexpected  because  none  of  other  reported
HBC derivatives assemble to form nanotubes in
acetone.   For  the  nanotubular  assembly  of   2,  an
acetone suspension of this HBC (1.5  10
4
M)
was heated  to 50C,  and the  resultant  clear  solu-
tion  was  allowed  to  cool   to  25C.   The  solu-
tion  gradually  became   turbid  and  displayed  a
red-shifted absorption spectrum characteristic of
J-aggregated HBCs (fig. S1, C and D). SEM of
an  air-dried  sample  of  the  suspension,   obtained
after a 12-hour incubation, showed the presence
of heavily bundled cylindrical nanostructures (fig.
S6A). TEM revealed that the cylinders are actu-
ally  nanotubes  (NT
2
)  with  a  uniform  diameter
of  20  nm  (fig.   S6B).
NT
1Cu
  dispersed  individually  in  acetone,
where  the  nanotubular  assembly  of  HBC  2  can
occur. As a typical example of the successful het-
erojunction  (Fig.   1C),   the  acetone  dispersion
of  NT
1Cu
,  used  as  the  seed (Fig.  1B),  was  pre-
sonicated  for  5  to  10  min  so  that  the  nanotubes
were cut into short pieces for enhancing the prob-
ability   of   linear   heterojunction   (fig.   S3C).   The
resultant   dispersion  of   NT
1Cu
  (1.5    10
4
M,
1.0 ml) was mixed at 50C with an acetone solu-
tion  of  HBC  2  (1.5    10
4
M,   1.0  ml).   When
the  mixture  was  allowed  to  cool   and  stand  at
25C,   the  assembly  of  HBC  2  took  place.  The
self-assembly of  2 without  NT
1Cu
 gave rise to a
suspension  of   bundled  NT
2
.   However,   the  co-
assembling  mixture  in  the  presence  of   NT
1Cu
remained clear even after 12 hours. When an air-
dried sample of this clear dispersion was studied
by  SEM,   micrometer-long  nanotubular   objects
with  bright   and  dark  segments   were  observed
(Fig. 2A and fig. S7). Most of the nanotubes ap-
peared  to  consist   of   two  block  segments,   but
some  were  composed  of  three  block  segments.
Likewise, scanning TEM allowed for visualiz-
ing the presence of segments with different con-
trasts in single nanotubes (Fig. 2C). By means of
element  mapping  using  TEM  energy-dispersive
x-ray  spectroscopy  (TEM-EDX),  we  confirmed
that   copper   is  localized  in  the  bright   segments
(Fig. 2, E and F), whereas carbon populates over
the  entire  nanotube  (Fig.  2,  D  and  F).  These  ob-
servations demonstrate the occurrence of  a linear
heterojunction  to  give   block-NT
1Cu
/NT
2
  (Fig.
1C). Considering the electronic characters of the
two HBC molecules, the heterotropic  p-stacking
interaction  seems  stronger  than  the  homotropic
one.   This   drives   the   preferential   assembly   of
HBC  2 on the nanotubular facets of seed  NT
1
.
Cu
.
Because multiblock heterojunction nanotubes such
as  NT
1Cu
NT
2
NT
1Cu
NT
2
 and  NT
1Cu
NT
2
NT
1Cu
 were not detected, postconnection of  NT
2
with  NT
1Cu
 is unlikely. In tapping-mode atomic
force microscopy (AFM) on a silicon wafer, these
two  block  segments   exhibited  different   height
profiles, 16 to 18 nm and 8 to 10 nm (Fig. 2B),
Fig. 2. Microscopic imaging of block-NT
1Cu
/NT
2
 ([2]/[1] = 1.0). The sample was prepared by drop-casting
its  acetone  dispersion  and  air  dried.  (A)  SEM  (scale  bar,   500  nm),   (B)  tapping-mode  AFM  (scale  bar,
200 nm), and (C) scanning TEM (scale bar, 50 nm) micrographs. TEM-EDX mapping of (D) carbon (scale
bar, 50 nm), (E)  copper (scale  bar, 50  nm), and  (F)  carbon  and copper  elements (scale bar, 50 nm).
Fig. 1. Molecular structures of HBCs 1 and 2 and schematic illustrations of the preparation of (A) NT
1
(bundled)  by  MeOH  vapor  diffusion  into  a  THF  solution  of  HBC  1,  (B)  seed  NT
1Cu
  (dispersed)  by  post-
functionalization of NT
1
 with Cu(OTf)
2
 in MeOH, and (C) block-NT
1Cu
/NT
2
 (dispersed) by cooling a hot
acetone  solution  of   HBC  2  in  the  presence  of   NT
1Cu
  as  the  seed.   (D)   Schematic  illustration  of   an
idealized  cross  section  of  block-NT
1Cu
/NT
2
  at  the  heterojunction  interface.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   341
REPORTS
that were the same as those observed for sepa-
rately   prepared   homotropic   NT
1Cu
  and   NT
2
(fig.  S8).  The  exceptionally  small  height  profile
of   NT
2
  indicates  a  low  structural  robustness  of
its  graphite-like  wall   because  of   the  nonplanar
HBC  core  of  2  (fig.  S5).
As shown in fig. S9,  NT
1
 (black solid curve)
and  NT
2
  (black  broken  curve),   when  photoex-
cited at 365 nm, fluoresced most intensely at 585
and  594  nm,   respectively  (16,   18,   29).   In  sharp
contrast,   NT
1Cu
  luminesced  much  less  intensely
(fig.   S9,   red)   as  a  consequence  of   possible  flu-
orescence quenching by Cu
2+
in the coordination
network  around  the  nanotube.   These  contrasting
luminescence  features  allowed  us  to  investigate
whether   the   two  graphite-like   nanotubular   seg-
ments  in  block-NT
1Cu
/NT
2
  (Fig.   1C)  communi-
cate with one another by excitation energy transfer
over  the  heterojunction  interface.  When  an  ace-
tone  dispersion  of   block-NT
1Cu
/NT
2
  prepared
by using the mole ratio [2]/[1] of 0.5 for the step-
wise  coassembly  was  photoexcited  at   365  nm,
the  observed  fluorescence  (Fig.  3B,  pink)  was
as   weak  as   that   of   homotropically  assembled
NT
1Cu
  (Fig.  3B,  red).  Even  when  the  mole  ra-
tio [2]/[1] used for the stepwise coassembly was
increased  from  0.5  to  1.0  (orange),  1.5  (green),
and  2.0  (blue)  (Fig.   3A),   the  fluorescence  in-
tensity  of  block-NT
1Cu
/NT
2
  remained  almost
unchanged at a very low level (Fig. 3B). In con-
trast to  block-NT
1Cu
/NT
2
 (Fig. 3B inset), a mix-
ture  of   homotropic   NT
1Cu
  and  NT
2
  ([2]/[1]   =
1.0)  (Fig.   3C,   orange)  displayed  a  rather  bright
fluorescence (Fig. 3D inset), where the observed
intensity  was  the  sum  of   those  of   NT
1Cu
  and
NT
2
 (Fig. 3D, orange). When the mixing ratio of
NT
2
 to  NT
1Cu
 was varied ([2]/[1] = 0.5 to 2.0)
(Fig. 3C), the overall fluorescence intensity changed
depending  on  the  amount  of  NT
2
  (Fig.  3D).  To-
gether   with  the  results   of   these  control   experi-
ments,  the  fluorescing  properties  observed  for
block-NT
1Cu
/NT
2
  indicate  that  the  NT
1Cu
  and
NT
2
 segments communicate efficiently over the
heterojunction interface (Fig. 1D) by excitation en-
ergy  transfer.   The  results  also  suggest   that   the
amount of unconnected  NT
2
, if any formed in the
stepwise coassembly (Fig. 1C), is negligibly small.
Because  the  excitation  energy  transfers  over
the   heterojunction   interface   from  one   nanotu-
bular   segment   (NT
2
)   to  the  other   (NT
1Cu
)   in
block-NT
1Cu
/NT
2
 (Fig. 1C), we were motivated
to  explore  the  behaviors  of  charge  carriers,   if
generated,   in  block-NT
1Cu
/NT
2
.   For   this   pur-
pose,   we  used  a  flash-photolysis  time-resolved
microwave conductivity (FP-TRMC) method (30),
which  allows  for   evaluating  the  intrinsic  prop-
erties  of   charge  carriers  without   electrodes.   At
first,   we   investigated  the   FP-TRMC  profiles
of   homotropically  assembled   NT
1Cu
  and   NT
2
.
Upon  laser   excitation  at   355  nm  (photon  den-
sity, 4.7  10
15
cm
2
), both nanotube samples in
the solid state displayed TRMC signals, indicat-
ing  that   these   nanotubes   are   photoconductive.
The  TRMC  signals thus observed for  NT
1Cu
 and
NT
2
  decayed  at   comparable  rates  (fig.   S10,   A
and B) with lifetimes (t
1/e
) of 1.4  10
6
and 2.5 
10
6
s,  respectively  (Fig.  4).  Of  particular  inter-
est to note here, the charge carriers generated in
block-NT
1Cu
/NT
2
  ([2]/[1]   =   1.0)   were   long-
lived  (fig.   S10D):   The  observed  lifetime  (t
1/e
  =
8.8    10
6
s)  was  roughly  five  times  longer  than
those  of   NT
1Cu
  and  NT
2
  (Fig.   4).   Taking  into
account   the  energy  levels  of   1  (16)  and  2  (fig.
S11)   estimated  from  their   electrochemical   and
spectral   data,   it   is  most   likely  that   the  NT
1Cu
and  NT
2
  segments  preferentially  accommodate
hole and electron, respectively. As a consequence
of such preferential localization of hole and elec-
tron   in   block-NT
1Cu
/NT
2
,   the   probability   of
charge recombination could be reduced. In sharp
contrast,  a mixture of homotropic  NT
1Cu
 and  NT
2
([2]/[1] = 1.0) (fig. S10C) hardly showed suppres-
sion of charge recombination (t
1/e
 = 2.0  10
6
s)
(Fig.  4).
The  behaviors   of   excitons   and  charge  car-
riers  thus  observed  for  semiconducting  block-
NT
1Cu
/NT
2
  are  remarkable   considering  that
they are brought about only by noncovalent con-
nection  of  two  different  homotropic  blocks  with
Fig.  3.  (A) Absorption and  (B)  fluorescence spectra  in acetone at 25C of  block-NT
1Cu
/NT
2
  prepared
by  using  different  molar  ratios  of  2  to  1  for  their  stepwise  coassembly  {[1]  =  1.5    10
4
M;  [2]  =  0
(red), 0.75  10
4
M (pink), 1.5  10
4
M (orange), 2.3  10
4
M (green), and 3.0  10
4
M (blue)}. (B
inset)   A  photograph  of   an  acetone   dispersion  of   block-NT
1Cu
/NT
2
  ([2]/[1]   =  1.0)   upon  365-nm
excitation.  (C)  Absorption  and  (D)  fluorescence  spectra  in  acetone  at  25C  of  mixtures  of  NT
1Cu
  and
NT
2
 at different molar ratios of 2 to 1 {[1] = 1.5  10
4
M; [2] = 0 (red), 0.75  10
4
M (pink), 1.5 
10
4
M (orange), 2.3  10
4
M (green), and 3.0  10
4
M (blue)}. (D inset) A photograph of an acetone
suspension of a mixture of NT
1Cu
 and NT
2
 ([2]/[1] = 1.0) upon 365-nm excitation. The baseline uprise
in  (C)  upon  increment  of  [2]  is  due  to  light  scattering  by  bundled  NT
2
.
Fig. 4. Lifetimes (t
1/e
) of charge carriers generated
by  laser   excitation  of   NT
1Cu
,   NT
2
,   a  mixture  of
NT
1Cu
 and NT
2
 ([2]/[1] = 1.0), and block-NT
1Cu
/NT
2
([2]/[1] = 1.0) in the solid state.  t
1/e
 is defined by the
time when the FP-TRMC transient decays down to 1/e
of its maximum value (fig. S10).
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 342
REPORTS
an  extremely  thin  (~3  nm)   facet.   In  particular,
the  nearly  perfect   fluorescence  quenching  of   its
NT
2
  block  substantiates  that  electronic  effects
of  heterojunctions  can  indeed  propagate  over  a
micrometer-long  distance  through  a  great  number
of  p-stacks in semiconducting organic materials.
References  and  Notes
1.   M.   T.   Bjrk  et  al.,   Nano  Lett.   2,  87  (2002).
2.   S.   Banerjee,   S.  S.   Wong,   Nano  Lett.  2,   195  (2002).
3.   O.   Harnack,   C.   Pacholski,   H.   Weller,   A.   Yasuda,
J.   M.   Wessels,   Nano  Lett.   3,   1097  (2003).
4.   B.   Tian  et  al.,   Nature  449,   885  (2007).
5.   A.   I.   Hochbaum,   P.   Yang,   Chem.   Rev.   110,  527  (2010).
6.   F.-S.  Tsai   et  al.,   Appl.   Phys.  Express  4,   025002  (2011).
7.   S.   Gnes,   H.   Neugebauer,   N.   S.  Sariciftci,   Chem.   Rev.
107,  1324  (2007).
8.   B.   C.   Thompson,   J.   M.   J.   Frchet,   Angew.   Chem.   Int.   Ed.
47,   58  (2008).
9.   G.   Yu,   J.   Gao,   J.   C.  Hummelen,  F.   Wudl,   A.   J.   Heeger,
Science  270,   1789  (1995).
10.   P. Peumans, S. Uchida, S. R. Forrest, Nature 425, 158 (2003).
11.   G.   Li   et  al.,   Nat.   Mater.   4,   864  (2005).
12.   J.   Y.   Kim  et  al.,   Science  317,   222  (2007).
13.   T.   F.   A.   De  Greef  et  al.,   Chem.  Rev.   109,   5687  (2009).
14.   F.   J.   M.   Hoeben,  P.   Jonkheijm,   E.   W.   Meijer,   A.   P.   H.   J.
Schenning,   Chem.   Rev.   105,  1491  (2005).
15.   F.   Wrthner  et  al.,  J.  Am.  Chem.  Soc.  126,  10611
(2004).
16.   Y.   Yamamoto  et  al.,   Science  314,  1761  (2006).
17.   A.  L.  Sisson  et  al.,  Angew.  Chem.  Int.  Ed.  47,  3727  (2008).
18.   Y.   Yamamoto  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.   106,
21051  (2009).
19.   N.   Sakai,   R.   Bhosale,   D.   Emery,   J.   Mareda,   S.   Matile,
J.   Am.   Chem.   Soc.   132,  6923  (2010).
20.   By using crystallizable core units, the formation of rodlike
block  co-micelles  has  been  demonstrated  (2124).
21.   X.   Wang  et  al.,   Science  317,  644  (2007).
22.   T.   Gdt,   N.  S.   Ieong,   G.   Cambridge,   M.   A.   Winnik,
I.   Manners,   Nat.   Mater.   8,  144  (2009).
23.   J.   B.   Gilroy  et  al.,   Nat.   Chem.  2,   566  (2010).
24.   S.   K.   Patra  et  al.,   J.   Am.   Chem.   Soc.   133,  8842
(2011).
25.   J.   P.   Hill   et  al.,   Science  304,  1481  (2004).
26.   W.   Jin  et  al.,   J.   Am.   Chem.   Soc.   130,  9434  (2008).
27.   Materials  and  methods  are  available  as  supporting
material   on  Science  Online.
28.   W.  Zhang,  W.  Jin,  T.  Fukushima,  N.  Ishii,  T.  Aida,  Angew.
Chem.   Int.   Ed.  48,   4747  (2009).
29.   G.   Zhang  et  al.,   J.   Am.   Chem.   Soc.   129,  719
(2007).
30.   A.   Saeki,   T.   Fukumatsu,   S.   Seki,   Macromolecules  44,
3416  (2011).
Acknowledgments:   We  thank  E.  Ohta  (RIKEN)  for  DFT
calculation  of  HBC  2.   W.Z.   thanks  the  Japan  Society  for
the  Promotion  of  Science  Young  Scientist  Fellowship
(219925).  T.F.  thanks  Ministry  of  Education,  Culture,
Sports,   Science,   and  Technology,   Japan,   for  financial
support  (21350108).
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/340/DC1
Materials  and  Methods
Figs.   S1  to  S11
References  (3133)
27  June  2011;   accepted  14  September  2011
10.1126/science.1210369
Dynamics  of   the  Reaction  of   Methane
with  Chlorine  Atom  on  an  Accurate
Potential   Energy  Surface
Gbor  Czak*  and  Joel  M.  Bowman
The reaction of the chlorine atom with methane has been the focus of numerous studies that
aim to test, extend, and/or modify our understanding of mode-selective reactivity in polyatomic systems.
To this point, theory has largely been unable to provide accurate results in comparison with experiments.
Here, we report an accurate global potential energy surface for this reaction. Quasi-classical trajectory
calculations using this surface achieve excellent agreement with experiment on the rotational
distributions of the hydrogen chloride (HCl) product. For the Cl + CHD
3
 HCl + CD
3
 reaction at low
collision energies, we confirm the unexpected experimental finding that CH-stretch excitation is no more
effective in activating this late-barrier reaction than is the translational energy, which is in contradiction
to expectations based on results for many atom-diatom reactions.
D
ecades   of   experimental   and  theoretical
studies of atom-diatom reactions led to a
well-validated  framework  for  predicting
the effect of vibrational excitation on the ensuing
dynamics (1, 2). Earlier fundamental research dem-
onstrated  the  importance  of  the  reaction  barrier
location  on  the  efficacy  of  partitioning  the  total
energy between internal excitation of the diatomic
molecule and relative translational  energy of the
reactants. The careful and correct analysis of these
reactions  led  to  the  Polanyi   rules  (3),   which
state that vibrational energy is more efficient than
is translational energy in activating a late-barrier
reaction, whereas the reverse is true for an early-
barrier reaction. Recent studies have investigated
the generality and validity of these paradigms for
polyatomic  systems.   The  X  +  methane  (CH
4
and deuterated isotopologues) reactions (which
replace the diatomic with a five-atom molecule)
have  played  a  central   role  in  this   research,   in
which, for example, the choice of X as H, O, F,
and Cl  has  permitted  the height and location  of
the  reaction  barrier  to  vary  widely.  Recent  ex-
periments by Liu and co-workers (48) on the F
and Cl + methane reactions have uncovered sur-
prising departures from expectations that present a
strong challenge to theory, which ultimately pro-
vides detailed understanding of chemical reaction
dynamics. A rigorous theoretical approach to re-
action analysis consists of two components. The
first   is  to  determine  the  global  potential   energy
surface (PES) (9), which governs the nuclear mo-
tion,   and   the   second   is   to   perform  dynamics
calculations with the PES. We succeeded in carry-
ing  out   this   process   recently  for   the   early-low-
barrier F + CHD
3
 reaction, for which we were able
to  illuminate  the  surprising  experimental  result  of
the enhancement of the DF + CHD
2
 channel by
exciting  the  CH-stretch  (10,   11).  In  this  Report,
we take the same approach to address and inter-
pret   experiments   on  the   late-high-barrier   Cl   +
CHD
3
 reaction by Liu and co-workers (5), which
also uncovered a surprising result, namely that at
low  collision  energies  (E
coll
)  vibrational   excita-
tion of the CH-stretch was no more effective than
was translational energy in promoting the reaction.
This result, as pointed out by these authors, contra-
dicts   the   rule   of   thumb   of   reaction   dynamics
(Polanyi  rules).  Other  interesting  experimental  re-
sults of this reaction are also successfully addressed.
As  with  the  previous  accurate  PES  for  F  +
CH
4
 (10), the Cl + CH
4
 PES is a permutationally
invariant fit (12,  9) to roughly 16,000 high-level
ab initio electronic energies. The selection of con-
figurations  for the  PES is  quite similar to  proce-
dures  used  for  the  F  +  CH
4
  PES  (10,   12),   and
details  are  given  in  (13).   A  key  part  of  this  ap-
proach is the use of an electronic structure method
that  gives  accurate  energies,  especially  for  the
barrier height, reaction enthalpy, and the entrance
and exit channel van der Waals (vdW) wells. These
wells,   which  result   from  long-range  attractive
interactions,  are  ubiquitous  in  chemistry,  and  as
we show here, the prereactive one has a substan-
tial effect on the Cl + CHD
3
 reaction dynamics at
low collision energies. The inclusion of the spin-
orbit (SO) correction is also essential in the present
case because it effectively increases the barrier
height and reaction endoergicity by 0.8 kcal/mol
and has a substantial effect on the entrance chan-
nel vdW well. (The SO correction is a relativistic
effect,   which  lowers  the  energy  of  the  halogen
atoms and has about twice as large an energy shift
on the heavier Cl than on F. The widely applied
nonrelativistic  electronic  structure  computations
neglect  this  effect.)  There  is  also  a  substantial
basis setsuperposition error in this region, which
has to be corrected. Thus, the goal for the present
PES is to take all of this into account. In order to
achieve this goal, we used a composite electronic
structure  method,   which  provides   accurate  en-
ergies   with  affordable  computational   time.   The
general composite approach (14), which is wide-
ly used, combines results from several levels of
ab initio method and basis (15,  16). Second, in
order to account for the SO effect differences be-
tween the SOand non-SOground-state electronic
energies,  obtained  by  means  of  multireference
configuration interaction (MRCI) with Davidson
correction  (MRCI  +  Q)  with  basis  set  aug-cc-
pVTZ (MRCI + Q/aug-cc-pVTZ), were added to
Cherry L. Emerson Center for Scientific Computation and De-
partment of Chemistry, Emory University, Atlanta, GA 30322,
USA.
*To   whom  correspondence   should   be   addressed.   E-mail:
czako@chem.elte.hu
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   343
REPORTS
the  composite  non-SO  energies  at  1598  ClCH
4
configurations in the entrance channel, where the
SO  corrections  are  substantial  and  nonconstant.
(2000 Cl + CH
4
 fragment data were also shifted
by  the  constant   SO  correction  of  the  Cl   atom.)
Third, counterpoise correction for entrance chan-
nel   basis   setsuperposition  error   at   the  above-
mentioned 1598 configurations was applied. The
present PES is based on electronic energies with
basis set effects up to aug-cc-pCVTZ(correlation-
consistent polarized core-valence triple-zeta basis
augmented  with  diffuse  functions)  (17);  electron
correlation  up  to  the  gold  standard  CCSD(T)
(coupled-cluster with single and double and per-
turbative triple excitations) method (18); correla-
tion  effects  of  the  core-core  and  core-valence
electrons;   and  SO  and  counterpoise  corrections
for the entrance channel. As a result, this present
PES  corresponds  to  the  SO  ground  state,   ac-
curately describes the vdW regions both in the
entrance and exit channels, and describes both
the  abstraction  (HCl   +  CH
3
)   and  substitution
(H + CH
3
Cl) channels. Thus, it represents a con-
siderable  advance  over  previous  PESs  for  Cl  +
CH
4
, including  several  semiempirical  (19,   20)
and  ab  initiobased  surfaces  in  2  (21),  3  (22),
and 12(full) (23) dimensions.
Aschematic of the PES, given in Fig. 1, shows
the  stationary-point  structures  and  energies  of
the abstraction and substitution reactions Cl(
2
P
3/2
,
2
P) + CH
4
HCl + CH
3
 and H + CH
3
Cl, where
Cl(
2
P
3/2
)  is  the  SO  ground  state  of  the  Cl  atom
lying  below  the  non-SO  energy  of   Cl(
2
P)   by
0.8 kcal/mol. The vdWwells in the entrance chan-
nel   for   the  CHCl   and  HCCl   linear   bond  ar-
rangements are belowCl(
2
P
3/2
) + CH
4
(eq) by 0.3
and  0.6  kcal/mol,   respectively.   (That   the  most
favorable vdWorientation is the HCCl one is both
meaningful  and  easily  understood  from  a  simple
sum-of-pairs interaction because C is more polar-
izable than H.) The abstraction reaction has a late
(product-like) saddle-point of energy 7.6 kcal/mol
relative to Cl(
2
P
3/2
) + CH
4
(eq) and a vdW well
in the product channel with a dissociation energy
(D
e
)  of  2.4  kcal/mol.  The  PES  reaction  endoer-
gicity for the HCl + CH
3
 channel is 5.7 kcal/mol.
These values are in excellent agreement with our
benchmark energies of 7.6, 2.4, and 6.0 kcal/mol,
respectively,   which  were  obtained  by  using  the
focal-point analysis (FPA) approach (14) [see com-
putational   details  in  (24)].   The  PES  reaction  en-
doergicity  is  also  in  excellent  agreement  with  the
experimental value, deduced tobe 6.0 kcal/mol (13).
None of the previous PESs are as accurate in
all  of  these  key  energies.  In  particular,  focusing
on the important entrance and exit channel vdW
wells,  the  present  PES  contains  an  accurate  de-
scription  of  the  latter,  (CH
3
HCl),  with  a  sub-
stantial   D
e
  value  of  2.4  kcal/mol.  This  contrasts
with the conclusion based on a semiempirical PES
with  a  D
e
  of  0.3  kcal/mol  that   the  existence  of
this product complex is questionable (20). With
respect  to  the  entrance  channel  vdW  well,  there
are  even  greater   contrasts  with  previous  PESs.
This vdW region in particular is affected by SO
2
P   0.8 
2
P
3/2
   0
H + CH
3
Cl
HCl + CH
3
6.0 (5.7)
3.6 (3.3)
Cl + CH
4
7.6 (7.6)
  0.3
25.2 (26.0)
42.1 (43.0)
  0.6
(CH
3
---HCl)
vdW
(H--CH
3
--Cl)
SP
(CH
3
--H--Cl)
SP
Reaction coordinate
R
e
l
a
t
i
v
e
 
e
n
e
r
g
y
 
(
k
c
a
l
/
m
o
l
)
Fig. 1. Schematic of the global SO and non-SO ground-state PESs of the Cl + CH
4
 reaction showing the
accurate  benchmark  energies  and  the  PES  values   in  parentheses;   for   example,   7.6  (7.6)   shows  the
excellent  agreement  between  the  benchmark  and  PES  barrier  heights.  All  the  energies  are  relative  to
the  SO  ground  state  Cl(
2
P
3/2
)  +  CH
4
(eq).  The  negative  energies  correspond  to  the  attractive  region  of
the  vdW  well  in  the  entrance  channel  on  the  SO  surface  (Fig.  2).
3.0 3.5 4.0 4.5 5.0 5.5 6.0 6.5 7.0 7.5 8.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
E
SO
3
SO
2
SO
1
A
1
MRCI+Q
H
3
CH---Cl (C
3v
)
E
n
e
r
g
y
 
(
k
c
a
l
/
m
o
l
)
2.5 3.0 3.5 4.0 4.5 5.0 5.5 6.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
E
A
1
SO
3
SO
2
SO
1
MRCI+Q
HCH
3
---Cl (C
3v
)
E
n
e
r
g
y
 
(
k
c
a
l
/
m
o
l
)
R(C---Cl) / 
3.0 3.5 4.0 4.5 5.0 5.5 6.0 6.5 7.0 7.5 8.0
A
1
SO
1
H
3
CH---Cl (C
3v
)
PES
2.5 3.0 3.5 4.0 4.5 5.0 5.5 6.0
SO
1
A
1
HCH
3
---Cl (C
3v
)
PES
R(C---Cl) / 
Fig. 2. Potential   energy  curves  of  CH
4
Cl  as  a  function  of  the  CCl  distance  along  the  C
3v
  axis  with
fixed CH
4
(eq) geometry and (top) CHCl or (bottom) HCCl linear bond arrangements that were (left)
computed  at  the  MRCI+Q/aug-cc-pVTZ  level   or  (right)  obtained  from  the  non-SO  and  SO-corrected
ground-state PESs. A
1
 and E denote the ground and excited non-SO electronic states, respectively, and
SO
1
,  SO
2
,  SO
3
  are  the  three  SO  states.  The  energies  are  relative  to  Cl(
2
P
3/2
)  +  CH
4
(eq).
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 344
REPORTS
interaction,  as  shown  in  Fig.  2,  where  potential
curves  both  with  and  without   SO  coupling  are
shown   for   the   entrance   channel.   Our   multi-
reference  configuration  interaction  results  show
that the non-SO electronic ground state potential
has  minima  with  CHCl   and  HCCl   bond  ar-
rangements with depths of 0.3 kcal/mol and 0.9
kcal/mol,   respectively  (25).   The  SO  interaction
has a minor effect  on the former, whereas it  de-
creases  the  depth  of  the  latter  by  0.3  kcal/mol;
but, the HCCl orientation still remains the deeper
minimum.   It   is   critical   that   the   present   PES
describes these vdWregions accurately, as shown
in Fig. 2, because they play an important role in
the low  E
coll
 dynamics. [Additional comparisons
between  the  PES  and  benchmark  properties,  in-
cluding  data  for   the  substitution  channel,   are
presented in (13).]
Having shown the high accuracy of the PES
by comparison with benchmark ab initio data, we
applied it to simulations of the collision dynamics
of  the  title  reaction.  We  performed  more  than  2
million quasi-classical trajectories (QCTs) for the
reactions of Cl(
2
P
3/2
) with CH
4
(v = 0), CHD
3
(v =
0), and CHD
3
(v
k
= 1) [k = 1, 3, 6, 5], where v = 0,
v
1
  =  1,   and  v
k
  =  1  [k  =  3,   6,   5]  denote  the  vi-
brational ground state, CH-stretch, and three dif-
ferent   bend  excitations,   respectively.   Details  of
the QCTcalculations are given in (13). Classical
zero-point leak and vibrational energy relaxation
fromv
k
= 1 was investigated thoroughly for CHD
3
and  found  not   to  be  a  serious  issue,   as  already
reported in (8, 11) and discussed further in (13).
All   the  results  presented  below  correspond  to
the SO-corrected PES. Computations on the non-
SO  PES  show  that  the  inclusion  of  the  SO  cor-
rection in the PES decreases the cross sections by
Fig.  3.  Computed  and  experimental   HCl
rotational distributions for the Cl + CH
4
 re-
action at a collision energy of 3.7 kcal/mol.
Theory  uses  quasi-classical  trajectory  calcu-
lations on the SO-corrected PES considering
trajectories  in  which  CH
3
  has  at least  zero-
point vibrational energy. Experimental data
are taken from(28). On the basis of analysis
of two batches of trajectories, the estimated
statistical   uncertainty  of   the  computed
results is less than 15%.
Fig. 4. (A) Computed cross sections for the ground
state  (v  =  0)  and  reactant  CH-stretch  (v
1
  =  1)  and
bend (v
k
 = 1) [k = 3, 6, 5] excited Cl + CHD
3
(v)   
HCl  +  CD
3
  reactions  and  (B)  their  ratios  as  a  func-
tion  of   E
coll
.   (C)  Cross  section  ratios  at  equivalent
amount of total energy (E
tot
 = E
coll
 + E
v
), where the
vibrational energies (E
v
) are 0, 8.6, and 3.0 kcal/mol
(relative to zero-point energy) for the ground state
and  stretch-   and  bend-excited  reactions,   respec-
tively.   (Right)   Snapshots   of   a  nonreactive  Cl   +
CHD
3
(v
1
  =  1)   trajectory  illustrating  the  stereo-
dynamics in the vdW region causing the unexpected
s
v
/s
g
 < 1 ratio at E
tot
 = 9.6 kcal/mol, as seen in (C).
Cl + CHD
3
(v
1
=1)
E
coll
 = 1.0 kcal/mol
0   2   4   6   8   10   12   14   16   18   20
0
10
20
30
40
50
60
0   2   4   6   8   10  12  14  16  18  20
0
1
2
3
4
v
6
=1
v
3
=1
v
5
=1
v
6
=1
v
3
=1
v
5
=1
v
1
=1
E
coll
 (kcal/mol)
v
 
/
 
g
0   2   4   6   8   10   12   14   16   18   20
0
1
2
3
4
5
v
3
=1
v
5
=1
v
6
=1
v
1
=1
v=0
Cl + CHD
3
(v) > > > > HCl + CD
3
E
coll
 (kcal/mol)
 
(
b
o
h
r
2
)
6   8   10   12   14   16   18   20
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
v
3
=1
v
6
=1
v
5
=1
v
1
=1
v
 
/
 
g
E
tot
 (kcal/mol)
A
B
C
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   345
REPORTS
a factor of 1.5 to 2.5 at low  E
coll
 because of the
increase  in  the  barrier  height,  but  it  has  no  sub-
stantial effect on the final state distributions.
First,   consider   the  HCl(v  =  0,   J )   rotational
distributions  for  the  Cl   +  CH
4
(v  =  0)  reaction.
These were reported by three experimental groups
showing  extremely  cold  rotational   populations
(2628). Theoretical simulations have been strug-
gling to reproduce this rotational distribution for
many years; the previous work overestimates the
rotational   temperature   of   the   HCl   product   en-
semble  (19,   23,   29).  In  Fig.  3,  we  present  QCT
results obtained by using the present PES and, as
seen,  the  agreement  between  theory  and  experi-
ment (27,  28) is excellent. We also computed the
HCl rotational distributions for Cl + CHD
3
(v
1
 = 1)
showing   cold   rotational   distribution   of   the
stretch-excited  product  HCl(v  =  1,   J ),   similar
to HCl(v = 0,  J ) from Cl + CH
4
(v = 0), and sub-
stantially  hotter   rotational   temperature  of   the
vibrationally   ground   state   HCl   in   qualitative
agreement with an older experiment (which had
large uncertainties) (30).
Next, we considered the effect of vibrational
excitation in CHD
3
, mentioned already. The Polanyi
rules (3) state that for late-barrier (atom+ diatom)
reactions, the reactant vibrational energy is more
efficient than is the translational energy in sur-
mounting the barrier. However, as noted already
a recent crossed molecular beam experiment (5)
found  that   this  picture  could  not  be  simply  ex-
tended for the Cl + CHD
3
reaction. To investigate
this finding, we calculated cross sections for the
reactant  ground  state  and  bend  and  CH-stretch
excited Cl + CHD
3
(v
k
) HCl + CD
3
 reactions
and  show  the  results  in  Fig.   4  as  a  function  of
both  E
coll
  and  total   energy  (E
tot
).   At   the  same
value  of   E
coll
,   we  see  that   all   the  bending  and
especially the CH-stretch excitations enhance the
reaction relative to Cl + CHD
3
(v = 0) (Fig. 4, A
and B). Thus, in this sense there is enhancement
of   the   reaction  by  excitation  of   these   modes.
However,  as  noted  in  the  experimental  study,  at
the same E
tot
translational energy is more effective
than  the  excitation  of  the  reactive  CH-stretch  or
bend  at  low  E
coll
.  As  the  E
coll
  increases,  the  in-
tuitively  expected  enhancement   of   reactivity  is
seen upon vibrational excitation. This is best seen
by plotting cross section ratios (s
v
/s
g
) as a func-
tion of  E
tot
 (Fig. 4C). As seen,  s
v
/s
g
 is less than
1 if the  E
tot
 is below 11 and (15, 15, 9) kcal/mol
for the CH-stretch and (v
3
, v
6
, v
5
) bending modes,
respectively. Only CD
3
(v =0) products were probed
experimentally, whereas theory shows the total re-
activity.  Correlating  the QCT cross sections  to
CD
3
(v = 0) results in a decrease of the s
CH
/s
ground
ratio, improving the agreement with the measured
data (fig. S1). Furthermore, the experiment applied
thermal  bending excitation; thus, the measured
bending cross sections show the average effect
of the three bending modes (5). Theory predicts
that the  v
5
(e) (CD
3
 deformation) bending mode
is  the  most  efficient  to  drive  the  reaction  (Fig.
4B), similar to F + CHD
3
. Overall, both theory and
experiment   show  that   the  same  amount   of   total
energy distributed among different nuclear motions
has different effects on chemical reactivity.
In order to gain insight into these results, we
examined the trajectories for the ground and stretch-
excited CHD
3
at the same E
tot
of 9.6 kcal/mol, thus
corresponding to a lowE
coll
 for CHD
3
(v
1
= 1). We
determined  the  distributions  of  the  smallest  H-Cl
and  C-Cl   distances   for   nonreactive  trajectories
and, as shown in fig. S2, most of the trajectories
for the CH-stretchexcited reaction do not reach
the transition state. Instead, the Cl atomturns back
at the vdWregion in the r
C-Cl
 = 2.9 to 3.5 range.
This occurs because at low  E
coll
, the CHD
3
 rotates
to the energetically favorable, but nonreactive,
H-CCl orientation (Fig. 4, right). Thus, at lowE
coll
the entrance channel vdWwell orients the reactants
in an unreactive configuration. At higher collision
energies, this effect is diminished, and the expected
enhancement of the reaction for the stretch-excited
CHD
3
 (over translational energy) is seen.
Next, we considered the experimental results
on the vibrational distribution of HCl (5). As noted
in (5), vibrationally adiabatic theory predicts that
the  ground  state  and  CH-stretchexcited  Cl   +
CHD
3
 reactions produce exclusively HCl(v = 0)
and  HCl(v  =  1)   products,   respectively.   Experi-
ment found the breakdown of this simple theory
for   the  excited  reaction  because  the  measured
fraction of HCl(v = 1), correlated to CD
3
(v = 0),
was only 45%(5). Our dynamics calculations show
that at higher E
coll
, above the energetic threshold for
HCl(v = 1), the ground-state reaction still produces
mainly HCl(v = 0), and the fraction of HCl(v = 1) is
only 1% with only a slight  E
coll
 dependence. This
small ratio increases to about 2% if the results are
correlated  to  CD
3
(v  =  0),  which  is  in  quantitative
agreement  with  experiment  (5).  The  reactant  CH-
stretch excitation increases the fraction of HCl(v =1)
to  10%  and  30  to  50%  for all  the  CD
3
  states  and
CD
3
(v  =  0),   respectively,   which  is  again  in  good
agreement   with   the   above-mentioned   correlated
experiment   (5).   The   computations   support   the
experimental observation: The ground state reaction
is vibrationally adiabatic, whereas the CH-stretch
excited reaction is nonadiabatic.
Last to be considered was the very recent ex-
periment (6) on steric control of Cl +CHD
3
(v
1
=1).
We have performed QCTcalculations with aligned
CHD
3
(v
1
 = 1) in which the CH-stretch is parallel
or   perpendicular   to  the  initial   relative  velocity
vector  of  the  reactants.   We  found  that   the  total
reactivity  of   H-abstraction  is   higher   at   parallel
alignment  relative  to  that  at  perpendicular  ori-
entations, which is in agreement with experiment
(6).   The  trajectories  show  that   the  initial   orien-
tation  is   maintained  while  the  Cl   approaches
CHD
3
(v
1
 = 1), supporting the recent experiment
(6). However, at the turning point the QCTs show
substantial energy transfer causing rotational ex-
citation  of   CHD
3
,   and  the  prealignment   is  not
conserved after the collision (Fig. 4, right).
References  and  Notes
1.   L.   Che  et  al.,   Science  317,   1061  (2007).
2.   D.   Skouteris  et  al.,   Science  286,   1713  (1999).
3.   J.   C.   Polanyi,   Science  236,  680  (1987).
4.   J. J. Lin, J.  Zhou,  W. Shiu, K.  Liu,  Science 300,  966 (2003).
5.   S.  Yan,  Y.-T.   Wu,   B.   Zhang,   X.-F.   Yue,   K.   Liu,   Science
316,   1723  (2007).
6.   F.   Wang,   J.-S.   Lin,   K.   Liu,   Science  331,   900  (2011).
7.   W.  Zhang,  H.  Kawamata,  K.  Liu,  Science  325,  303  (2009).
8.   G.  Czak,  Q.  Shuai,  K.  Liu,  J.  M.  Bowman,  J.  Chem.  Phys.
133,   131101  (2010).
9.   J.  M.  Bowman,  G.  Czak,  B.  Fu,  Phys.  Chem.  Chem.  Phys.
13,  8094  (2011).
10.   G.   Czak,   B.  C.   Shepler,   B.  J.   Braams,   J.   M.   Bowman,
J.   Chem.   Phys.  130,   084301  (2009).
11.   G. Czak, J. M. Bowman, J. Am. Chem. Soc. 131, 17534 (2009).
12.   B.   J.   Braams,   J.   M.   Bowman,   Int.   Rev.   Phys.  Chem.   28,
577  (2009).
13.   Materials  and  methods  are  available  as  supporting
material   on  Science  Online.
14.   A.  G.  Csszr,  W.  D.  Allen,  H.  F.  Schaefer,  J.  Chem.  Phys.
108,   9751  (1998).
15.   The  composite  energies  were  obtained  as  E[UCCSD( T)/
aug-cc-pVDZ]  +  E[AE-UMP2/aug-cc-pCVTZ]     E[UMP2/
aug-cc-pVDZ],  where  AE  denotes  correlating  all  the
electrons.  For  the  entrance  channel,  counterpoise  and
spin-orbit  corrections  were  computed  at  the  AE-UMP2/
aug-cc-pCVTZ  and  MRCI+Q/aug-cc-pVTZ  levels  of  theory,
respectively.  The  PES  was  represented  by  a  polynomial
expansion in y
ij
 = exp(r
ij
/a) (where a = 2 bohr), including
all   terms  up  to  total  degree  six.  3262  coefficients  were
determined  by  a  weighted  linear  least-squares  fit  of
roughly  16,000  energy  points.  The  root  mean  square
(RMS)fitting  errors  are  0.2,  0.4,  and  1.0  kcal/mol  for
energy intervals (0, 31), (31, 63), and (63, 143), respectively.
16.   For  15  arbitrary  geometries  with  energies  in  the  wide
0  to  36  kcal/mol   range,   we  found  that  this  composite
method  gives  results  comparable  with  extremely
high-quality  all-electron  CCSD(T)/aug-cc-pCVQZ
calculations  with  a  RMS  of  only  0.4  kcal/mol,   whereas
the  RMS  error  of  high-level   CCSD(T)/aug-cc-pVTZ
calculations  is  1.1  kcal/mol.   Furthermore,   the  composite
method  reduces  the  computational   time  by  factors  of
about  1000  and  5  relative  to  the  above-mentioned
high-level   computations,   respectively.
17.   K.   A.   Peterson,  T.   H.   Dunning  Jr.,   J.  Chem.  Phys.   117,
10548  (2002).
18.   K. Raghavachari, G. W. Trucks, J. A. Pople, M. Head-Gordon,
Chem.  Phys.  Lett.  157,  479  (1989).
19.   J. C. Corchado, D. G. Truhlar,  J. Espinosa-Garca,  J. Chem.
Phys.   112,  9375  (2000).
20.   C.  Rangel, M.  Navarrete,  J.  C.  Corchado,  J.  Espinosa-Garca,
J.  Chem.  Phys.  124,  124306  (2006).
21.   S. T. Banks, D. C. Clary, Phys. Chem. Chem. Phys. 9, 933 (2007).
22.   H.-G.   Yu,   G.   Nyman,   J.   Chem.   Phys.   111,  6693  (1999).
23.   J.   F.   Castillo,  F.   J.   Aoiz,   L.  Baares,   J.   Chem.   Phys.   125,
124316  (2006).
24.   The  benchmark  FPA  study  considers  extrapolation  to  the
complete  basis  set  limit  using  aug-cc-pVnZ  [n  =  5  and  6]
bases, electron correlation beyond CCSD(T), core correlation
effects,  scalar  relativistic  effects,  and  spin-orbit  corrections.
25.   These  relative  energies  are  benchmarked  at  the
highly  accurate  CCSD(T)/aug-cc-pCVQZ  level   of  theory
correlating  all   the  electrons,   including  corrections
for  the  basis  set  superposition  error.
26.   W.   R.   Simpson,  T.   P.   Rakitzis,   S.   A.   Kandel,   T.   Lev-On,
R.   N.   Zare,   J.  Phys.   Chem.   100,  7938  (1996).
27.   D. F. Varley, P. J. Dagdigian, J. Phys. Chem. 99, 9843 (1995).
28.   C.   Murray,   B.   Retail,   A.   J.   Orr-Ewing,   Chem.   Phys.  301,
239  (2004).
29.   S. J. Greaves et al., Phys. Chem. Chem. Phys. 13, 11438 (2011).
30.   W.  R.  Simpson,  T.  P.  Rakitzis,  S.  A.  Kandel,  A.  J.  Orr-Ewing,
R.  N.  Zare,  J.  Chem.  Phys.  103,  7313  (1995).
Acknowledgments:  G.C.  thanks  the  National  Science
Foundation  (grant  CHE-0625237),  and  J.M.B.  thanks
the U.S. Department of Energy (grant DE-FG02-97ER14782)
for  financial  support.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/343/DC1
Materials  and  Methods
Figs.   S1  to  S3
Tables  S1  to  S3
17  May  2011;   accepted  9  September  2011
10.1126/science.1208514
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 346
REPORTS
800,000  Years  of  Abrupt
Climate  Variability
Stephen  Barker,
1
*  Gregor  Knorr,
2
R.  Lawrence  Edwards,
3
Frdric  Parrenin,
4,5
Aaron  E.   Putnam,
6
Luke  C.  Skinner,
7
Eric  Wolff,
8
Martin  Ziegler
1
We  constructed  an  800,000-year  synthetic  record  of  Greenland  climate  variability  based  on  the
thermal  bipolar  seesaw  model.  Our  Greenland  analog  reproduces  much  of  the  variability  seen  in
the  Greenland  ice  cores  over  the  past  100,000  years.  The  synthetic  record  shows  strong  similarity
with  the  absolutely  dated  speleothem  record  from  China,  allowing  us  to  place  ice  core  records
within  an  absolute  timeframe  for  the  past  400,000  years.  Hence,  it  provides  both  a  stratigraphic
reference  and  a  conceptual  basis  for  assessing  the  long-term  evolution  of  millennial-scale  variability
and  its  potential  role  in  climate  change  at  longer  time  scales.  Indeed,  we  provide  evidence  for  a
ubiquitous association between bipolar seesaw oscillations and glacial terminations throughout the
Middle  to  Late  Pleistocene.
I
ce core records from Greenland first demon-
strated the existence of repeated, large, abrupt
shifts  in  Northern  Hemisphere  climate  dur-
ing  the  last   ice  age  (1,   2).   These  shifts  are  one
expression  of  a  global  system  that  is  capable  of
driving  major  changes  in  climate  components
such  as  ocean  temperatures  (3,   4)  and  monsoon
rainfall   (5).   The  Greenland  records  provide  an
archetypal  view  of  abrupt  climate  variability  (6)
over  the  last   glacial   cycle,   which  was  character-
ized  by  rapid  alternations  between  cold  (stadial)
and  warmer   (interstadial)   conditions   [known  as
Dansgaard-Oeschger (D-O) oscillations]. But iron-
ically, the very high temporal resolution of these
records makes it difficult to look farther back in
time;  the high  accumulation  rates  on  the  Green-
land  ice  sheet   mean  that   more  than  3000  m  of
ice  may  represent  just  100,000  years  of  climate
history.   Fortunately,   climate  records  preserved  in
Antarctic  ice  (7)  enable  us  to  address  this  funda-
mental  problem.
The  thermal  bipolar  seesaw  model  (8,   9)  at-
tempts to explain the observed relationship between
millennial-scale temperature variability observed
in  Greenland  and  Antarctica  by  calling  on  var-
iations in the strength of the Atlantic meridional
overturning   circulation   (AMOC).   The   north-
ward heat transport associated with this circulation
(10) implies that changes in the strength of over-
turning should lead to opposing temperature  re-
sponses in either hemisphere. According to the
seesaw  model,  a  transition  from  weak  to  strong
AMOCwould cause an abrupt warming across the
North  Atlantic  region  (a  D-O  warming  event)
while  temperatures  across  Antarctica  would  (in
general) shift fromwarming to cooling. The ocean-
atmosphere  climate  system  is  an  integrated  and
synergistic system, and it is important to note that
the overall concept of the bipolar seesaw we in-
voke here is not restricted to oceanic processes but
also  includes  atmospheric  shifts  that   may  be  re-
lated to the variations we are interested in(9, 1114).
According   to   the   thermal   bipolar   seesaw
model, we should observe an antiphase relation-
ship  between  the  Greenland  temperature  anom-
aly and the rate of change of Antarctic temperature
(9). This can be illustrated by a lead/lag analysis
of  the  methane-tuned  temperature  records  after
removal of their orbital time scale variability (6)
(Greenland,   GL
T
_hi,   and   Antarctica,   AA
T
_hi)
and the first time derivative of Antarctic temper-
ature, AA
T
_hi (Fig. 1).  Comparison of the undif-
ferentiated  records  illustrates  the  historical   debate
as to whether the two signals are  positively cor-
related,   with  a  southern  lead  of   1000  to  1600
years, or negatively correlated, with the north lead-
ing  by  400  to  800  years  (15,   16).   However,   as
implied  in  (9)  and  illustrated  in  Fig.   1,   a  near
zero-phase  anticorrelation  is   observed  between
GL
T
_hi   and  AA
T
_hi.   Uncertainties   in  the   ice
agegas  age  offset  (Dage),  which  may  be  up  to
hundreds  of years (17), mean that an exact  anti-
phase relationship is unlikely to be observed (6).
As  described  by  (18)  using  a  similar  approach,
the  process  of  differentiating  amplifies  noise  in
the  original  temperature  record.  Smoothing  the
record  of  AA
T
_hi  before  differentiating  reduces
this  noise  but   will   compromise  the  ability  of
AA
T
_hi  to  replicate  the  abrupt  nature  of  D-O
warming  events  and  reduce  the  predicted  ampli-
tude  of  smaller  events.  The  choice  of  smoothing
window is therefore a trade-off between these ef-
fects  (6)  (Fig.  1).
The empirical relations illustrated in Fig. 1 of-
fer the possibility of producing a synthetic record
of  Greenland  climate  using  the  Antarctic  record,
with  the  purpose  of   reconstructing  the  nature
of  northern  variability  beyond  the  present   limit
of  the  Greenland  records.  The  record  of  Green-
land  temperature  (GL
T
)  is  broken  down  into  its
orbital   and   millennial   time   scale   components,
GL
T
_lo and GL
T
_hi, respectively (Fig. 2 and fig.
S5), where GL
T
_lo is  a 7000-year smoothing of
GL
T
  (6)   and  GL
T
_hi   is  the  difference  between
GL
T
and GL
T
_lo. We consider GL
T
_hi as the north-
ern  temperature  anomaly  with  respect   to  mean
background  conditions.   Building  on  Fig.   1,   we
assume   that   the   rate   of   Antarctic   temperature
change  is  inversely  proportional  to  the  northern
temperature anomaly. We therefore scale the am-
plitude  of  AA
T
_hi  to  match  that   of  GL
T
_hi   to
produce a synthetic record of northern millennial-
scale temperature variability, GL
T
_syn_hi (Fig. 2C)
(6). It can be seen that a synthetic reconstruction
of GL
T
could be made by combining GL
T
_syn_hi
with  an  estimate  for   GL
T
_lo.   The  orbital   time
scale  components  of   the  Greenland  and  Ant-
arctic  temperature records (GL
T
_lo  and  AA
T
_lo,
respectively) are highly correlated, with the south-
ern  record  leading  the  north  by  ~2000  years
(6).  We  therefore  incorporate  longer time scale
variations  into  our  reconstruction  by  substitut-
ing  GL
T
_lo  with  a  scaled  version  of   AA
T
_lo,
shifted by 2000 years (which we call GL
T
_syn_lo)
(fig.   S5)  (6).   Our  full  reconstruction,  GL
T
_syn
(Fig.   2D),   is  then  the  sum  of   GL
T
_syn_lo  and
GL
T
_syn_hi.
Our  formulation  of  the  thermal   bipolar  see-
saw concept is qualitatively analogous to that of
(9)  in  that  it  implies  the  existence  of  a  heat  reser-
voir  that  convolves  the  northern  signal,  produc-
ing a southern signal with a longer characteristic
time  scale.  Our  approach  is  slightly  different  in
that   we  relate  the  rate  of  Antarctic  temperature
change directly to the northern temperature anom-
aly.   Indeed,   we  note  that   for  some  long  stadial
events,   particularly  those  associated  with  gla-
cial terminations, Antarctic temperatures appear to
rise  unabated  until  an  abrupt  warming  event  oc-
curs   in  the  north  (19).   On  the  other   hand,   our
formulation does not imply that Antarctic temper-
atures  must   continue  to  rise  indefinitely  when-
ever Greenland is cold, only while it is cold with
respect   to   background   conditions   (defined   by
the  orbital  time  scale  component).  We  also  note
that  northern  temperature  (regardless  of  back-
ground conditions) is not always constant through-
out stadial events. For example, Greenland warmed
significantly  during  cold  stadial   21  (Fig.   2D).
By  our  formulation,  the  rate  of  Antarctic  tem-
perature  rise  during  this  event  would  decrease
correspondingly,   in  line  with  observations  (Fig.
2A)  (20).
We used a thresholding approach for predict-
ing the occurrence of abrupt Greenland warming
events  based  on  minima  in  the  second  time  dif-
ferential of AA
T
 (AA
T
) (Fig. 2, E and F). This
has an advantage over use of the first differential
(decreasing through zero) because it is capable of
distinguishing  between  events   of   varying  mag-
nitude  and  incorporates   information  about   con-
ditions before and after an abrupt event (6). Using a
relatively insensitive threshold (blue dashed line in
Fig.   2F),   we  are  able  to  identify  the  largest  D-O
1
School of Earth and Ocean Sciences, Cardiff University, Cardiff
CF10 3AT, UK.
  2
Alfred Wegener Institute, 27570 Bremerhaven,
Germany.
  3
Department   of   Earth  Sciences,   University  of   Min-
nesota, Minneapolis, MN 55455, USA.
  4
Laboratoire de Glaciologie,
CNRS and Joseph Fourier University, 38400 Grenoble, France.
5
Laboratoire Chrono-Environnement, 25000 Besanon, France.
6
Department  of  Earth  Sciences  and  Climate  Change  Institute,
University  of   Maine,   Orono,   ME  04469,   USA.
  7
Godwin  Lab-
oratory   for   Palaeoclimate   Research,   Department   of   Earth
Sciences,  University  of  Cambridge,  Cambridge  CB2  3EQ,  UK.
8
British   Antarctic   Survey,   Madingley   Road,   High   Cross,
Cambridge  CB3  0ET,  UK.
*To   whom  correspondence   should   be   addressed.   E-mail:
barkers3@cf.ac.uk
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   347
REPORTS
temperature shifts recorded in Greenland, whereas
smaller  events,   such  as  D-O  2,   require  a  more
sensitive  threshold  (red  line).  Accordingly,  we  are
able  to  identify  almost  all  of  the  canonical  D-O
events  over  the  past  90,000  years  without  intro-
ducing  spurious events. We incorporate a cor-
rection,  based  on  the  time  integrated  per  55-cm
sample of ice (7), to account for loss of temporal
resolution in the deeper parts of the ice core (6).
Our synthetic reconstruction of Greenland tem-
perature  closely  resembles  the  observed  record
in  terms  of  both  its  timing  and  the  structure  of  in-
dividual events (Fig. 2). This is despite probable
variability in the relationships between  d
18
O [for
the Greenland Ice Sheet Project 2 ice core (GISP2)]
or   dD  [for  the  European  Project  for  Ice  Coring
in  Antarctica  Dome  C  ice  core  (EDC)]   versus
local   temperature  through  time  (21)   and  other
millennial-scale  variability  that  might  not  be  re-
lated to the bipolar seesaw. We find similar results
using  alternative  Antarctic  ice  core  records  (6).
On the basis of the predictive ability of GL
T
_syn
over the past ~100,000 years, we can extend our
reconstruction back to ~800,000 years ago (Fig.
3  and  Fig.  4).  In  doing  so  we  implicitly  assume
that   the   empirical   relationships   observed   over
the last  glacial  cycle held  during earlier  periods.
Given  the  inherent   uncertainty  in  this  assump-
tion,   we   do   not   claim  particular   skill   at   pre-
dicting  the  absolute  amplitude  of  earlier  events;
however,  we  do  suggest  that  to  the  extent  that
the  underlying  physical mechanisms did persist
throughout   the   past   800,000  years,   the  timing
and  overall  structure  of  events  will  be  relatively
robust.
To test this hypothesis, we compared our syn-
thetic  reconstructions  with  real   climate  records.
The record of Asian monsoon variability derived
from cave deposits (speleothems) in China (5,  22)
is one of the best candidates for this task (Fig. 3).
The  Chinese  speleothem  d
18
O  record  is  thought
to  represent   changes  in  the  proportion  of  low
d
18
O  (summer  monsoon)  rainfall  within  annual
totals  (22)  and  can  be  considered  a  measure  of
the amount of summer monsoon rainfall or mon-
soon intensity. The combined record from several
deposits taken from a number of caves provides
a  continuous,   absolutely  dated  record  over   the
past   ~400,000  years  (22).   The  record  is  domi-
nated  by  orbital  time  scale  changes,  possibly  re-
lated to the influence of boreal summer insolation
on  the  strength  of  the  Asian  monsoon  (6).   Re-
moval   of   this  variability  by  normalizing  to  the
insolation  curve  (6)  reveals  distinctive  millennial
time  scale  activity  that  has  been  shown  to  cor-
respond  with  D-O  variability  over   Greenland
during  the  last  glacial  cycle  (5,   22).  This  corre-
spondence is thought to be caused by latitudinal
shifts  in  the  position  of  the  Intertropical  Con-
vergence  Zone  (ITCZ)  and  related  atmospher-
ic  phenomena  in  response  to  variations  in  the
AMOC and related changes in North Atlantic
temperature  (11).
There is  a strong one-to-one correspondence
between inferred weak-monsoon events and our
reconstructed  cold  events  in  Greenland  (Fig.  3).
Moreover,   there  are  pronounced  similarities   in
the  structure of abrupt  events, particularly during
deglacial   episodes   (terminations);   the   multiple
weak-monsoon   events   associated   with   glacial
terminations  of  the  Late  Pleistocene  (22)  are  re-
flected  by  multiple  cold  events  in  our   records.
Our   reconstruction  suggests   the   occurrence   of
large-amplitude  D-Otype oscillations between
160,000  and  180,000  years  ago  [during  marine
isotope stage 6 (MIS 6)] (Fig. 3). These may be
compared  with  similar  events  in  the  records  of
planktonic   d
18
O  and  tree  pollen  from  a  marine
3 2 1 0 1 2 3
0.2
0
0.2
0.4
0.6
0.8
1
Lag (kyr)
North leads South leads
B
Methane
C
o
r
r
e
l
a
t
i
o
n
C
o
r
r
e
l
a
t
i
o
n
North leads South leads
3 2 1 0 1 2 3
0.8
0.4
0.4
0.8
Lag (kyr)
0
1000yr
700yr
200yr
C
Vs AA
T
_hi
-10
0
10
30 40 50 60 70 80
A
A
T
_
h
i
 
(
)
Age (kyr) (EDC3)
-0.05
0
0.05
-0.01
0
0.01
-0.01
0
0.01
-2
0
2
G
L
 
T
_
h
i
 
(
)
-100
0
100
E
D
C
 
C
H
4
(
p
p
b
v
)
 
-100
0
100
G
I
S
P
 
C
H
4
(
p
p
b
v
)
A
Fig.   1.   Ice  core  records  from  Greenland  (GISP2)  and  Antarctica  (EDC)  (all   records  have  orbital   time
scale  variability  removed;  kyr,  thousands  of  years).  (A)  Methane  (17,  25)  with  tuning  points  (crosses)
used  to  place  all  records  on  the  EDC3  age  model  (26),  Greenland  temperature  (GL
T
_hi  with  200-year
smoothing)   derived  from  d
18
O  of   ice  (2),   and  Antarctic  temperature  (AA
T
_hi,   200-year   smoothing)
from  dD  of  ice  (7).  First  derivatives  of  AA
T
_hi  (AA
T
_hi)  are  shown  for  various  smoothing  lengths  (in  brackets)  of  the  undifferentiated  record.  (B)  Lead/lag
correlation  of  the  methane records suggests successful tuning  of  the  gas records.  (C)  Lead/lag  correlations  between GL
T
_hi, AA
T
_hi,  and  AA
T
_hi  reveal  the
well-known  relation  between  northern  and  southern  temperature  records  and  the  antiphase  relationship  between  GL
T
_hi  and  AA
T
_hi.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 348
REPORTS
Fig.   2.   Reconstructing   millennial-scale   climate
variability over Greenland using the Antarctic tem-
perature record. (A) The record of  dD from the EDC
ice  core  (AA
T
)   (7)   with  a  7000-year  smoothing  of
the  same  record  (AA
T
_lo).   (B)  Removal   of  orbital
time  scale  variability  and  application  of   a  700-
year smoothing (6) produces AA
T
_hi. (C) AA
T
_hi is
differentiated  and  then  scaled  to  GL
T
_hi   (green
curve)  to  produce  GL
T
_syn_hi  (orange  curve).   (D)
A  synthetic   reconstruction  of   Greenland  temper-
ature  variability  (GL
T
_syn;   red  curve)   constructed
by   adding  GL
T
_syn_hi   to  GL
T
_syn_lo  (6).   Green
curve is GISP2  d
18
O placed on EDC3 via methane
tuning (Fig. 1). (E and F) Minima in AA
T
 below a
threshold  (dashed  lines)   are  used  to  predict   the
occurrence of major warming events in Greenland
(F), identified by the corresponding colored dots in
(E). A threshold value of   1.2  10
5
(red dashed
line and dots) has good success at picking canon-
ical   D-O  events   [green  numbers   in  (D)   and  (E)]
without  introducing  spurious  events.
1
2
3
4   5
6
  7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
0
1 2 3 4 5 6 7 8 91011 1213 14151617 18 19 20 21 22 0
10 20 30 40 50 60 70 80 90
Age kyr (EDC3)
Age kyr (EDC3)
10 20 30 40 50 60 70 80 90
GL
T
E
-44
-40
-36
G
L
 
T
 
(
 
1
8
O
,
 
)
D
GL
T
_syn
-2x10
-5
0
2x10
-5
F
-10
0
10
B
A
A
T
_
h
i
-450
-430
-410
-390
E
D
C
 
D
 
(
)
A
AA
T
AA
T
_lo
-4
-2
0
2
4
C
GL
T
_hi
GL
T
_syn_hi
G
L
 
T
 
_
h
i
Fig. 3. (A to H) Compari-
son of reconstructed Green-
land climate variability with
other  records.  The  normal-
ized  record  of   monsoon
variability from China (A)
(5, 22), marine records from
the   Iberian  Margin  [(C)
to (E)] (23,  32), and the
record of atmospheric CH
4
(G)  (25)  share  many  fea-
tures  in  common  with  our
records   derived   from  the
Antarctictemperaturerecord
[(B) and (F)]. Colored dots
in  (H)  represent   the  oc-
currence  of   D-O  events
predicted from AA
T
 using
a  fixed  (red)  or  variable
(blue)  threshold  (6).  All
records  are  on  the  EDC3
time scale (26) except the
monsoon  record  which  is
on  its  own  absolute  time
scale(22). Thepollenrecord
from  MD95-2042  (32)  (C)
was placed on EDC3 by tun-
ing the corresponding plank-
tonic  d
18
O record (24) to
GL
T
_recon. Gray bars indi-
cate   cold   conditions   and
periods of weak monsoon.
Glacial terminations are indicated by Roman numerals.
400
500
600
700
C
H
4
 
(
p
p
b
v
) G -40
-35
-30
G
L
 
T
_
s
y
n
 
(
)
F
120 140 160 180 200 220 240 260
Age (kyr)
0
20
40
T
r
e
e
 
p
o
l
l
e
n
 
(
%
)
E
20
40
60
M
e
d
i
t
e
r
r
a
n
e
a
n
p
o
l
l
e
n
 
(
%
)
D
1
2
3
p
l
a
n
k
t
o
n
i
c
 
1
8
O
 
(
)
C
-4
0
4
G
L
T
_
s
y
n
_
h
i
 
(
)
B
S
p
e
l
e
o
t
h
e
m
 
1
8
O
(
n
o
r
m
a
l
i
z
e
d
)
A
H
T-II T-III
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   349
REPORTS
sediment core taken from the Iberian Margin (23).
On  the  basis  of  the  findings  of  Shackleton  et   al.
(24),   the  Iberian  Margin  records  were  tuned  to
the  EDC  dD  record  via  the  record  of   benthic
d
18
O  from  the same core  (23).  The tuning  exer-
cise  did  not   involve  the  surface  records,   which
therefore  provide  a  quasi-objective   target  for
comparing with our reconstruction [which should
be aligned with the surface-ocean records accord-
ing  to  (24)],   and  there  is  good  agreement  in  the
timing  and  structure  of  the  abrupt  events  during
MIS  6.   We  also  note  good  agreement   between
our reconstructions and the record of atmospheric
CH
4
 (25). Our predicted D-O warming events are
generally  aligned  with  sharp  increases   in  CH
4
(similar  to  the  observed  relationship  during  MIS
3). This relationship holds for the entire 800,000-
year record (Fig. 4) and provides critical ground-
truthing  for  our  reconstruction.
Building  on  previous  studies  (22),   we  used
the precise and absolutely dated Chinese speleo-
them  record  to  place  our   reconstruction  on  an
absolute  time  scale  for   the  past   400,000  years.
We  did  this  by  aligning  the  cold  events  in  our
reconstruction  with  the  inferred  weak-monsoon
events in the speleothem record (Fig. 4) (6). The
EDC3  age  scale  (which  remains  the  fundamen-
tal   basis  for  our  model)  was  derived  through  a
combination  of   ice  flow  modeling  and  various
age markers, including orbital tuning constraints
(26).   By  tuning  the  millennial-scale  features  of
GL
T
_syn to the speleothem record, we provide
a  refinement   of  the  age  scale  that   provides  an
Fig.   4.   (A  and  B)   800,000
years  of   abrupt   climate  varia-
bility. Records of North Atlantic
IRD (4), monsoon rainfall (5, 22)
(normalized)   and   SST   from
the   Iberian   Margin   (27)   all
show  strong  similarities  with
our reconstruction of Greenland
climate   variability   (GL
T
_syn_hi
and  GL
T
_syn).   Glacial   termi-
nations (identified by Roman
numerals) are characterized by
cold  conditions   across  Green-
land   and   the   North   Atlantic
and  weakened  monsoon  rain-
fall,  with  a  corresponding  rise
in  atmospheric  CO
2
  (33),   fol-
lowed  by  an  abrupt   warming
over Greenland, strengthening
of the monsoon, and sharp rise
in  atmospheric  CH
4
  (25).   Pink
boxes  indicate  terminal  North-
ern  Hemisphere   cold  periods.
Red and blue dots are predicted
D-O  warming  events  using  a
fixed or variable threshold, re-
spectively. Lowermost curves in
each  panel   are  moving  win-
dows  of  the  standard  devia-
tion of AA
T
_hi, our   bipolar
seesaw  activity  index  (note
that  orbital   time  scale  varia-
tions have been removed; blue
is 5000-year window; green is
10,000-year window). Increased
millennial-scale activity is gen-
erally  observed  during  transi-
tions between climate states,
with minimal activity during
interglacials and glacial max-
ima. All records are on the new
Speleo-Age  (A)  or  the  EDC3
(B) time scale except the ben-
thic  d
18
O stack (LR04) of (34),
which is on its own time scale.
TI TII TIIIA TIII TIV
TV TVI TVII
400
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21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 350
REPORTS
alternative  to  the  ultimate  dependence  on  orbital
tuning.  In  addition  to  providing  an  absolute  time
scale for the ice and gas records from Antarctica,
we  can  also  use  our   absolutely  dated  Green-
land reconstruction  as a tuning target for other
high-resolution paleo-records, such as records
of ice-rafted debris (IRD) from a North Atlantic
sediment   core  (4)   and  a  record  of   sea  surface
temperature  (SST)   from  a  core  off   the  Iberian
Margin  (27)  (Fig.  4).  Each  of  these  records  has
been  tuned  to  our  reconstruction  on  its  absolute
time  scale  (6).
Our synthetic records confirm that millennial
time  scale variability  and  abrupt  climate oscilla-
tions  occurred  in  Greenland  throughout  the  past
800,000  years,   and  more  specifically  they  sug-
gest that the underlying physical mechanisms rep-
resented by the conceptual thermal bipolar seesaw
were  relatively  invariant  throughout  this  period.
In  line  with  observations  for  the  last   glacial   pe-
riod (28), our reconstructions suggest that higher-
amplitude variability and more frequent D-Olike
warming events occurred when climate was in
an  intermediate  state  or   during  the  transitions
between  states  (Fig.   4).   Extending  the  observa-
tions  of  (22),   we  find  that   glacial   terminations
of   the   Middle   to   Late   Pleistocene   in   general
were  characterized  by  oscillations of  the  bipolar
seesaw.
This   apparently  ubiquitous   association  of
millennial-scale  climate  variability  with  glacial
terminations raises an important question: Is this
mode of variability a necessary component of de-
glacial climate change, or merely a complicating
factor? Previous studies (28,  29) have suggested
that  D-Otype  variability  might  represent  an  in-
herent resonance of the climate system, attaining
a  high  amplitude  only  within  certain  windows
of  opportunity  (i.e.,  intermediate  climate  states).
Given that global climate must pass through such
a  window  during  deglaciation,   one  could  argue
that terminal oscillations of the bipolar seesaw are
merely  a  symptom  of  deglacial   climate  change
(29). However, the precise correspondence observed
between bipolar seesaw oscillations and changes
in  atmospheric  CO
2
  during  glacial   terminations
(Fig. 4) suggests that the bipolar seesaw may play
more  than  just  a  passive  role  in  the  mechanism
of deglaciation (i.e., through the positive feedbacks
associated with increasing CO
2
) (14,  19,  22). With
the  supercritical  size  of  continental  ice  sheets  as
a possible precondition (30), and in combination
with  the  right  insolation  forcing  (31)  and  ice  al-
bedo feedbacks, the CO
2
 rise associated with an
oscillation  of   the  bipolar  seesaw  could  provide
the  necessary  additional  forcing  to  promote  de-
glaciation.   In  this  sense,   the  overall  mechanism
of  glacial  termination during the  Middle to  Late
Pleistocene  might   be  viewed  as  the  timely  and
necessary interaction between millennial and or-
bital  time  scale  variations.
References  and  Notes
1.   W.   Dansgaard  et  al.,   Science  218,  1273  (1982).
2.   M.   Stuiver,   P.   M.   Grootes,   Quat.   Res.  53,   277
(2000).
3.   G.   Bond  et  al.,   Nature  365,  143  (1993).
4.   J. F. McManus, D. W. Oppo, J. L. Cullen, Science 283, 971
(1999).
5.   Y.   J.   Wang  et  al.,   Nature  451,  1090  (2008).
6.   See  supporting  material   on  Science  Online.
7.   J.   Jouzel   et  al.,   Science  317,   793  (2007).
8.   W.   S.   Broecker,   Paleoceanography  13,  119  (1998).
9.   T.   F.   Stocker,  S.   J.   Johnsen,   Paleoceanography  18,  1087
(2003).
10.   K.   E.  Trenberth,  J.   M.   Caron,   J.   Clim.   14,  3433
(2001).
11.   M.   Vellinga,   R.   A.   Wood,   Clim.  Change  54,  251
(2002).
12.   J.   C.   H.   Chiang,   M.   Biasutti,   D.   S.  Battisti,
Paleoceanography  18,  1094  (2003).
13.   R.   F.   Anderson  et  al.,   Science  323,  1443  (2009).
14.   S.   Barker  et  al.,   Nature  457,  1097  (2009).
15.   A. Schmittner,  O. A. Saenko, A. J. Weaver,  Quat.  Sci. Rev.
22,  659  (2003).
16.   E.   J.   Steig,   R.   B.   Alley,   Ann.   Glaciol.   35,   451
(2002).
17.   T.   Blunier,   E.   J.   Brook,   Science  291,   109  (2001).
18.   M.   Siddall   et  al.,   Quat.  Sci.  Rev.   25,  3185  (2006).
19.   E.   W.   Wolff,   H.   Fischer,   R.   Rothlisberger,   Nat.   Geosci.   2,
206  (2009).
20.   E.   Capron  et  al.,   Quat.   Sci.   Rev.   29,  222  (2010).
21.   E.   Capron  et  al.,   Clim.   Past  6,  345  (2010).
22.   H.   Cheng  et  al.,   Science  326,  248  (2009).
23.   V.   Margari   et  al.,   Nat.  Geosci.   3,  127  (2010).
24.   N.   J.   Shackleton,   M.  A.   Hall,   E.  Vincent,
Paleoceanography  15,   565  (2000).
25.   L.   Loulergue  et  al.,   Nature  453,  383  (2008).
26.   F.   Parrenin  et  al.,   Clim.   Past  3,  485  (2007).
27.   B.   Martrat  et  al.,   Science  317,   502  (2007).
28.   M.   Schulz,   W.   H.   Berger,   M.   Sarnthein,   P.   M.   Grootes,
Geophys.   Res.   Lett.   26,   3385  (1999).
29.   A.  Sima,  A.  Paul,  M.   Schulz,  Earth  Planet.   Sci.  Lett.  222,
741  (2004).
30.   M.   E.  Raymo,   Paleoceanography  12,  577  (1997).
31.   J. D. Hays, J. Imbrie, N. J. Shackleton, Science 194, 1121
(1976).
32.   M. F. Snchez Goi, F. Eynaud, J. L. Turon, N. J. Shackleton,
Earth  Planet.  Sci.  Lett.  171,  123  (1999).
33.   D.   Lthi   et  al.,   Nature  453,   379  (2008).
34.   L.   E.  Lisiecki,  M.   E.  Raymo,   Paleoceanography  20,
PA1003  (2005).
Acknowledgments:   We  thank  the  authors  of  all   of  the
studies  cited  here  for  making  their  results  available  for
this  work.   Supported  by  a  Philip  Leverhulme  Prize  (S.B.),
Natural   Environment  Research  Council   (UK)  awards
NE/F002734/1 and NE/G004021/1 (S.B.),  and NSF grants
0502535  and  1103403  (R.L.E.).   This  study  is  also  part
of  the  British  Antarctic  Survey  Polar  Science  for  Planet
Earth  Programme,   funded  by  the  Natural   Environment
Research  Council   (UK).
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1203580/DC1
Materials  and  Methods
Figs.   S1  to  S14
Tables  S1  to  S3
References
31  January  2011;   accepted  26  August  2011
Published  online  8  September  2011;
10.1126/science.1203580
Pre-Clovis  Mastodon  Hunting  13,800
Years Ago at the Manis Site, Washington
Michael  R.  Waters,
1
*  Thomas  W.  Stafford  Jr.,
2,5
H.  Gregory  McDonald,
3
Carl  Gustafson,
4
Morten  Rasmussen,
5
Enrico  Cappellini,
5
Jesper  V.  Olsen,
6
Damian  Szklarczyk,
6
Lars  Juhl  Jensen,
6
M.  Thomas  P.  Gilbert,
5
Eske  Willerslev
5
The tip of a projectile point made of mastodon bone is embedded in a rib of a single disarticulated
mastodon  at  the  Manis  site  in  the  state  of  Washington.  Radiocarbon  dating  and  DNA  analysis
show that the rib is associated with the other remains and dates to 13,800 years ago. Thus, osseous
projectile  points,  common  to  the  Beringian  Upper  Paleolithic  and  Clovis,  were  made  and  used
during  pre-Clovis  times  in  North  America.  The  Manis  site,  combined  with  evidence  of  mammoth
hunting  at  sites  in  Wisconsin,  provides  evidence  that  people  were  hunting  proboscideans  at
least  two  millennia  before  Clovis.
R
ecent studies have strengthened the case
that the makers of Clovis projectile points
were  not   the  first   people  to  occupy  the
Americas  (15).   If  hunting  by  humans  was  re-
sponsible  for  the  megafauna  extinction  at   the
end  of   the  Pleistocene  (6),   hunting  pressures
must   have   begun  millennia   before   Clovis   (7).
Here we reexamine the evidence from the Manis
site in the state of Washington (8), an early mas-
todon  kill  that  dates  to  800  years  before  Clovis.
Between 1977 and 1979, a single male mas-
todon (Mammut  americanum) was excavated from
sediments   at   the   base   of   a   kettle   pond   at   the
Manis  site  (figs.   S1  to  S3)  (810).   Some  bones
were  spirally  fractured,   multiple  flakes  were  re-
moved  from  one  long  bone  fragment,  and  other
bones  showed  cut   marks  (8,   11,   12).   The  only
documented  artifact   associated  with  the  masto-
don was a foreign osseous  fragment, interpreted
as   the  tip  of   a  bone  or   antler   projectile  point,
1
Center for  the  Study  of  the  First  Americans,  Departments  of
Anthropology  and  Geography,   Texas   A&M  University,   4352
TAMU, College Station,  TX 778434352,  USA.
  2
Stafford Re-
search, 200 Acadia Avenue, Lafayette, CO 800261845, USA.
3
Park  Museum  Management  Program,  National  Park  Service,
1201 Oakridge Drive, Suite 150, Fort Collins, CO 80525, USA.
4
245 Southeast Derby Street, Pullman, WA 991632217, USA.
5
Centre  for  GeoGenetics,   University  of   Copenhagen,   ster
Voldgade  5-7,   1350  Copenhagen,   Denmark,
  6
Novo  Nordisk
Foundation  Center  for  Protein  Research,   Faculty  of  Health  Sci-
ences,  University  of  Copenhagen,  Blegdamsvej  3b,  2200 Co-
penhagen,   Denmark.
*To   whom  correspondence   should  be   addressed.   E-mail:
mwaters@tamu.edu
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   351
REPORTS
embedded  in  a  rib  fragment  that  was  recovered
ex  situ  from  sediments  excavated  when  a  back-
hoe uncovered the bone bed (Fig. 1 and fig. S4)
(8).   Organic  matter   associated  with  the  masto-
don  yielded  calibrated  radiocarbon  ages  of  ~14
thousand years ago (ka) (8,  10) (table S1). Over
the  past  35  years,  the  age  and  evidence  for  hu-
man involvement with the Manis mastodon have
been  challenged  (13).
We  obtained  13  accelerator  mass  spectrom-
etry (AMS)
  14
C dates from purified bone collagen
(4)  extracted  from  the  mastodon  rib  containing
the  embedded  osseous   object   and  from  both
tusks  (table  S2).  All  dates  were  statistically  iden-
tical  at  1  SD  and  establish  an  age  of  11,960  T
17
  14
C  years  before the  present  (yr B.P.)  for the
Manis mastodon (Table 1; average of four XAD
fractions; 13,860 to 13,765 calendar yr B.P.) (14).
These  dates  show  that  the  ex  situ  mastodon  rib
and  in  situ  skeleton  are  contemporaneous.
High-resolution x-ray computed tomography
(CT)   scanning   (15)   revealed   that   the   osseous
object embedded in the rib is dense bone shaped
to  a  point   (Fig.   1  and  movies  S1  and  S2).   The
point   penetrated  2.15  cm  into  the   rib;   the   tip
broke  after  entering  the  rib  and  separated  from
the main shaft. The combined length of the point
fragment   (tip  length  plus  the  length  of   the  em-
bedded  and  external  shaft  piece)  is  3.5  cm.
The rib with the embedded projectile point is
a  right  12th,  13th,  or  14th  rib  in  a  series  of  19,
but most likely the 14th rib (Fig. 2). The projec-
tile  point  entered  the  dorsal  surface  of  the  prox-
imal end of the rib immediately distal to the lateral
margins   of   the   two  articular   facets   at   approxi-
mately a 45 angle relative to the axis of the head
of  the  rib.   The  point   would  have  penetrated  the
hair   and  skin  and  about   25  to  30  cm  of   super-
ficial epaxial muscles (Fig. 2 and fig. S5). Thus it
was  at  least  27  to  32  cm  long,  comparable  with
the known length of later, Clovis-age thrown and
thrust  bone  points  (16).  There  is  no  evidence  of
bone growth around the point, indicating that the
mastodon  died  soon  after  it  was  attacked.
DNA  and  protein  sequencing  were  under-
taken  on  the  rib  and  bone  point  (supporting  on-
line  material  text  4  and  5).  Attempts  to  amplify
a  140base  pair  (bp)  fragment  of  the  16S  mito-
chondrial   DNA  (mtDNA)   from  the  rib  using
universal vertebrate primers (17) produced only
modern  (human)  contamination.   However,  re-
designing primers for a 69-bp fragment (including
primers,   table  S8)  of  D-loop  mtDNA  produced
sequences from both the rib and bone point that
were  identical   to  mastodon  and  distinct   from
other  proboscideans  (mammoth  or  elephant)  by
nine  substitutions.
We also obtained high-resolution tandem mass
spectrometry  (MS/MS)based  protein  sequences
from the projectile point and rib, and used another
mastodon  sample  as  a  second  reference  (tables
S3  to  S6).   The  MS/MS  spectra  from  the  bone
point   matched  the  reconstructed  mastodon  col-
lagen  sequences,   with  the  highest   scores  being
within a reference set of collagen sequences (table
S7  and  supporting  table  of   bone  point   marker
peptides).   These  results  and  controls  show  that
the  point  was  fashioned  from  mastodon  bone.
The  Manis  site  provides  further  evidence  of
a  human  presence  in  the  New  World  800  years
before Clovis [13 ka (4)] and shows that people
were   hunting   with   mastodon   bone   weapons
made from  earlier kills. Evidence for pre-Clovis
hunting  also  comes  from  the  14.2-ka  Schaefer
site and 14.8-ka Hebior site, Wisconsin (18,  19),
where   stone   artifacts,   but   no  projectile  points,
were found with the remains of mammoth (Mam-
muthus primigenius). Additional evidence of mega-
fauna hunting comes from sites where artifacts
are absent, but taphonomic evidence suggests hu-
man butchering, such as at the 13.8-ka Ayer Pond
site  (45SJ454),   Orcas  Island,   Washington  (20).
Studies  of   the  dung  fungal   spore  Sporormiella
from  lakes  in  Indiana  and  New  York  imply  that
megafauna  populations  collapsed  there  between
14.8 and 13.7 ka (7). Thus, the impact of human
hunters  on  the  North  American  megafauna  was
more prolonged than previously hypothesized and
was  not  a  Clovis  blitzkrieg  (21).  The  absence
of   stone   projectile   points   at   Manis,   Hebior,
Schaefer, and Orcas Island and the presence of
an osseous projectile point at Manis suggest that
osseous projectile points may  have been  the pre-
dominant  hunting  weapon  during  the  pre-Clovis
period.   Bone  and  ivory  points   and  other   tools
are  common  in  the  Upper  Paleolithic  of  Siberia
and in late Pleistocene sites in Beringia (2224).
They  are   durable   and  lethal   hunting  weapons
that continued to be used during and after Clovis
(16,  23,  25). The invention and spread of a new
hunting weapon at 13 kathe Clovis lithic point
may  have  accelerated  the  demise  of  or  doomed
the  last  megafaunal  species.
Table  1.  AMS
  14
C  ages  used  to  date  the  Manis  Mastodon.
Specimen  dated   Date  (
14
C  yr  B.P.   T  1  SD)   Lab  number   Material  dated
Mastodon  tusk  ivory
sample  no.  1
11,975  T  35   UCIAMS-11350   XAD-gelatin
(KOH  collagen)
Mastodon  tusk  ivory
sample  no.  1
11,975  T  35   UCIAMS-12046   XAD-gelatin
(KOH  collagen)
Mastodon  tusk  ivory
sample  no.  2
11,890  T  35   UCIAMS-11677   XAD-gelatin
(KOH  collagen)
Mastodon  rib  with
embedded  bone
projectile  point
11,990  T  30   UCIAMS-29113
XAD-gelatin
(KOH  collagen)
Average  of  four
radiocarbon
measurements
11,960  T  17
  14
C  yr  B.P.
(13,860  to  13,763  calendar  yr  B.P.)
   n  =  4
XAD-gelatin
(KOH  collagen)
0 1cm 0.5 
A
C
B
0 1 2 cm
0 1 2 cm
D
Fig.   1.  Mastodon  rib  with  the  embedded  bone  projectile  point.  (A)  Closeup  view.  (B)  Reconstruction
showing  the  bone  point  with  the  broken  tip.   The  thin  layer  represents  the  exterior  of  the  rib.   (C)  CT
x-ray showing the long shaft of the point from the exterior to the interior of the rib. (D) The entire rib
fragment  with  the  embedded  bone  projectile  point.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 352
REPORTS
References  and  Notes
1.   T.   Goebel,   M.   R.   Waters,   D.   H.   ORourke,   Science  319,
1497  (2008).
2.   M.   T.   P.   Gilbert  et  al.,   Science  320,   786  (2008).
3.   M.   R.   Waters  et  al.,   Science  331,   1599  (2011).
4.   M.  R. Waters, T. W. Stafford Jr., Science 315, 1122 (2007).
5.   T.   D.   Dillehay  et  al.,   Science  320,   784  (2008).
6.   P.   S.  Martin,  in  Quaternary  Extinctions,  a  Prehistoric
Revolution,   P.   S.  Martin,  R.   G.   Klein,   Eds.   (Univ.   of
Arizona  Press,   Tucson,   AZ,   1984),   pp.   354403.
7.   J.   L.   Gill,   J.   W.   Williams,   S.   T.   Jackson,   K.   B.   Lininger,
G.   S.   Robinson,   Science  326,  1100  (2009).
8.   C.   E.  Gustafson,  D.  Gilbow,  R.  Daugherty,  Can.  J.  Archaeol.
3,  157  (1979).
9.   K.   L.   Petersen,   P.   J.   Mehringer  Jr.,   C.  E.   Gustafson,
Quat.   Res.   20,  215  (1983).
10.   V.   E.  Morgan,   thesis,   Washington  State  University,
Pullman,   WA  (1985).
11.   D.   W.   Gilbow,   thesis,   Washington  State  University,
Pullman,   WA  (1981).
12.   A.   L.   Runnings,   thesis,   Washington  State  University,
Pullman,   WA  (1984).
13.   G.  Haynes,  The  Early  Settlement  of   North  America:
The Clovis Era (Cambridge Univ. Press, Cambridge, 2002).
14.   P.   J.   Reimer  et  al.,   Radiocarbon  51,  1111  (2009).
15.   T. M. Ryan, G. R. Milner, J. Archaeol. Sci. 33, 871 (2006).
16.   B.   A.   Bradley,   M.   B.   Collins,   C.   A.   Hemmings,
Clovis  Technology  (International   Monographs  in
Prehistory,   no.   17,  Ann  Arbor,   MI,  2010).
17.   P.   G.   Taylor,   Mol.   Biol.   Evol.   13,  283  (1996).
18.   D.   F.   Overstreet,   in  Paleoamerican  Origins:   Beyond
Clovis,  R.   Bonnichsen,   B.   T.   Lepper,   D.   Stanford,
M.   R.   Waters,  Eds.   (Center  for  the  Study  of  the  First
Americans,   Texas  A&M  University,   College  Station,   TX,
2005),  pp  183195.
19.   D.   J.   Joyce,   Quat.  Int.   142-143,  44  (2006).
20.   S.  M.  Kenady,  M.  C.  Wilson,  R.  F.  Schalk,  R.  R.  Mierendorf,
Quat.  Int.  233,  130  (2011).
21.   D.   K.   Grayson,   D.   J.   Meltzer,   J.  Archaeol.  Sci.  30,  585
(2003).
22.   T.   Goebel,   Evol.   Anthropol.   8,  208  (1999).
23.   R.   D.   Guthrie,   in  Animals  and  Archaeology:   Hunters  and
Their  Prey,  J.   Clutton-Brock,   C.   Grigson,   Eds.   (British
Archaeological   Reports  International   Series  163,   Oxford,
1983),  pp.   273294.
24.   C.   E.   Holmes,   Arctic  Anthropol.   38,   154  (2001).
25.   H.  Knecht,  in  Projectile  Point  Technology,  H.  Knecht,  Ed.
(Plenum,   New  York,   1997),   pp.   191212.
Acknowledgments:   We  thank  the  North  Star  Archaeological
Research  Program  established  by  J.  Cramer  and  R.  Cramer
and  the  Chair  in  First  Americans  Studies  for  funding.
We  thank  J.   Southon  for  providing  the  ultrafiltration
14
C  measurements.   Work  conducted  at  the  Center  for
GeoGenetics  was  supported  by  the  Danish  National
Research  Foundation.   E.C.  is  supported  by  the
European  Union  with  a  Marie  Curie  Intra  European
Fellowship  (grant  number  237227).  J.O.,   D.S.,  and
L.J.   are  supported  by  the  Novo  Nordisk  Foundation
Center  for  Protein  Research.  CT  scanning  was
performed  at  the  High  Resolution  X-ray  CT  Facility  at
the  University  of  Texas,   Austin.   J.   Halligan  prepared
the  illustrations.   T.   Jennings,   J.   Halligan,   T.   Goebel,
S.   Fiedel,   and  two  anonymous  individuals  reviewed
the  manuscript.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/351/DC1
SOM  Text
Figs.   S1  to  S5
Tables  S1  to  S8
References
Table  of  bone  point  marker  peptides
29  April   2011;   accepted  8  September  2011
10.1126/science.1207663
Fig.  2.  Anatomical position of the
Manis  rib.   (A)   Two  vertebrae  with
the  Manis  rib  inserted  into  its  cor-
rect  anatomical   position.  The  blue
arrow points to the embedded point
fragment. (B) Side view of mastodon
vertebrae with the Manis rib inserted
into  its  correct  anatomical   position,
with the trajectory of the point indi-
cated.  (C)  Mastodon  skeleton  show-
ing the location of ribs 12 to 14.
0 4 8 cm
transverse
processes
anterior 
posterior
p
o
i
n
t
 
t
r
a
j
e
c
t
o
r
y
point tip
A B
C
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   353
REPORTS
Information Transduction Capacity of
Noisy Biochemical Signaling Networks
Raymond Cheong,
1
Alex Rhee,
1
Chiaochun Joanne Wang,
1
Ilya Nemenman,
2
Andre Levchenko
1
*
Molecular  noise  restricts  the  ability  of  an  individual  cell  to  resolve  input  signals  of  different
strengths  and  gather  information  about  the  external  environment.  Transmitting  information
through complex signaling networks with redundancies can overcome this limitation. We developed
an  integrative  theoretical  and  experimental  framework,  based  on  the  formalism  of  information
theory,  to  quantitatively  predict  and  measure  the  amount  of  information  transduced  by
molecular  and  cellular  networks.  Analyzing  tumor  necrosis  factor  (TNF)  signaling  revealed  that
individual  TNF  signaling  pathways  transduce  information  sufficient  for  accurate  binary  decisions,
and  an  upstream  bottleneck  limits  the  information  gained  via  multiple  integrated  pathways.
Negative  feedback  to  this  bottleneck  could  both  alleviate  and  enhance  its  limiting  effect,
despite  decreasing  noise.  Bottlenecks  likewise  constrain  information  attained  by  networks
signaling  through  multiple  genes  or  cells.
S
ignaling networks are biochemical systems
dedicated to processing information about
the environment provided by extracellular
stimuli. Large populations of cells can accurately
sense signaling inputs, such as the concentration
of  growth  factors  or  other  receptor  ligands,   but
this task can be challenging for an individual cell
affected by biochemical noise (13). Noise maps
an input signal to a distribution of possible output
responses,   which  can  cause  loss  of  information
about   the  input.   For  example,   a  cell   cannot   re-
liably distinguish different inputs that, because of
noise, can generate the same output (Fig. 1A).
Conventional  metrics  related  to  the  standard
deviation or variance of the response distribution
measure  noise  magnitude  (48),   but  fail  to  elu-
cidate  how  noise  quantitatively  affects   the  ac-
curacy of information processing in single cells.
By  contrast,   an  information  theoretic  approach
(Fig. 1B), and the metric of mutual information in
particular, can quantify signaling fidelity in terms
of  the  maximum  number  of  input  values  that  a
cell   can  resolve  in  the  presence  of  noise.   Such
methods  have  been  commonly  used  to  evaluate
man-made telecommunication systems (9) and
more recently in computational neuroscience and
in  analyses  of transcriptional  regulatory  systems
(1014),  but  have  not  been  applied  to  biochem-
ical signaling networks. We developed a general
integrative theoretical and experimental frame-
work  to  predict  and  measure  the  mutual  infor-
mation  transduced  by  one  or   more  signaling
pathways. Applying this framework to analyze a
four-dimensional  compendium  of  single-cell  re-
sponses to tumor necrosis factor (TNF) (Fig. 1C,
see also SOM section 1), an inflammatory cyto-
kine  that  initiates  stochastic  signaling  at  physio-
logic  concentrations  spanning  about  four  orders
of magnitude (1521), shows that signaling via a
network  rather  than  a  single  pathway  can  abate
the information lost to noise. Furthermore, an in-
formation  bottleneck  can  restrict   the  maximum
information a network can capture, and negative
feedback potentially but not always relieves this
limitation.
The mutual information,  I(R;S), measured in
bits, is the binary logarithmof the maximumnum-
ber of input signal values (S), such as ligand con-
centrations,   that   a  signaling  system  can  perfectly
resolve  on  the  basis  of  its  noisy  output  responses
(R)  (9).  One  bit  of  information  can  resolve  two
different  signal  values,   2  bits  resolves  four  val-
ues, etc. More generally,
I(R;S)  =  
S
R
P(R,S)log
2
P(R,S)
P(R)P(S)
   
dRdS
1
1
Department  of  Biomedical  Engineering,  Johns  Hopkins  Uni-
versity, 3400 North Charles Street, Baltimore, MD 21218, USA.
2
Departments  of  Physics  and  Biology,  Emory  University,  400
Dowman Drive, Atlanta, GA 30322, USA.
*To   whom  correspondence   should   be   addressed.   E-mail:
alev@jhu.edu
A
B
C   D
Fig.  1.  Information theoretic analysis of cell signaling fidelity. (A) Schematic
showing information loss due to overlapping noisy response distributions. (B)
Diagram  of   the  TNFNF-kB  signaling  pathway  represented  in  biochemical
form  (left)  and  as  a  noisy  communication  channel  (right).  (C)  Experimental
flowchart for using immunocytochemistry to sample the conditional response
distribution at single-cell resolution and resulting four-dimensional compen-
dium  of   multiple   responses   in  cells   of   multiple   genetic   backgrounds   to
multiple TNF concentrations, at multiple time points. The data were collected
in  a  single  experiment,  allowing  controlled,  quantitative  comparisons  along
each  dimension.   (D)  Distributions  of  noisy  NF-kB  nuclear  translocation  re-
sponses to 30-min TNF exposure (examples shown at top) used to compute the
channel capacity of the TNFNF-kB pathway. Scale bars, 20  mm.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 354
REPORTS
The  joint  distribution  P(R,S)  determines  the
marginal distributions  P(R) and  P(S), and hence
also the mutual information, and can be decom-
posed as  P(R,S) =  P(S)  P(R|S). The response dis-
tribution,   P(R|S),  is  experimentally  accessible  by
sampling responses of individual isogenic cells to
various signal  levels (Fig.  1C),  and  its spread re-
flects   the   noise   magnitude   given   any   specific
input.   The  signal   distribution,   P(S),   reflects  po-
tentially  context-specific  frequencies  at   which  a
cell experiences different signal values. Although
the  amount  of  information  might  thus  vary  from
case to case, one can also determine the maximal
amount of transducible information, given the ob-
served  noise  (see  SOM section  2).  This quantity,
known  as  the  channel   capacity  (9),   is  a  general
characteristic   of   the   signaling   system  and   the
signal-response pair of interest and can thereby be
experimentally   measured   without   making   as-
sumptions  about  the  (possibly  nonlinear)  relation
between Rand S, signal power, or noise properties.
Using immunocytochemistry, we assayed nu-
clear   concentrations   of   the   transcription  factor
nuclear  factor   kB  (NF-kB)  in  thousands  of  in-
dividual mouse fibroblasts 30 min after exposure
to various TNFconcentrations (Fig. 1D). We chose
this time point because NF-kBtranslocation peaks
at   30  min  regardless  of  the  concentration  used,
initiating expression of early-response inflamma-
tory  genes  (1922).  The  NF-kB  response  value
in a single cell could yield at most 0.92 T 0.01 bits
of  information,   which  is  equivalent  to  resolving
2
0.92
= 1.9, or about 2, concentrations of the TNF
signal,   thus   essentially  only  reliably  indicating
whether TNF is present or not. (See SOM sec-
tions  2.2  and  3  regarding  the  low  experimental
uncertainty.) A bimodal input signal distribution,
P(S), with peaks at lowand high TNF concentra-
tions, maximizes the information (fig. S1), support-
ing the notion of essentially binary (digital) sensing
capabilities of this pathway (18), although we did
not observe bimodal output responses,  P(R|S).
Noise  also  limits  other  canonical   pathways,
including  signaling  by platelet-derived  growth
factor (PDGF), epidermal growth factor (23), and
G  proteincoupled  receptors  (24),  to  ~1  bit  (fig.
S2, A to C, and table S1). Even the most reliable
system  we  examined,   morphogen  gradient   sig-
naling through the receptor Torso in  Drosophila
embryos (25), was limited to 1.61 bits (fig. S2D
and  table  S1),  corresponding  to  about  three  dis-
tinguishable signal levels.
The pathways examined above are examples
of  individual  biochemical  communication  chan-
nels (Fig. 1B) that capture relatively lowamounts
of information about signal intensity, which would
allow only limited reliable decision making by a
cell. However, information in biological systems
is typically  processed by networks  comprising
multiple communication channels, each transduc-
ing information about the signal. For instance, a
transcription factor often regulates many genes,
a  receptor  many  transcription  factors,  and  a  dif-
fusible ligand many cells. The integrated outputs
of  such  multiple  channels  can  provide  more  in-
formation about the signal than the output of any
one channel (see SOM section 4). Subsequently,
downstream  signaling  processes  that   converge
to co-regulate common effectors, biological pro-
cesses,  or  physiologic  functions  can  provide  the
point needed to integrate the multiple outputs to
realize  the  benefit   of  increased  aggregate  infor-
mation (fig. S3). To provide a unified framework
for analyzing such various networks, we first the-
oretically investigated the information gained by
network signaling in general, then experimentally
tested  the  predictions  made  by  the  theory  when
applied to a specific system.
We considered two information theoretic mod-
els,  similar  to  models  of  population  coding  in
neural systems (2628), for transmitting a signal
S through multiple channels to the responses  R
1
,
R
2
,   ,   R
n
,   under   the  assumption  of   Gaussian
variables  (see  SOM  section  5).  The  bush  model
uses independent channels (topologically resem-
bling an upside-down shrub) (Fig. 2A), whereas
the  tree  model  signals  through a  common  chan-
nel   (trunk)   to  the  intermediate,   C,   before  di-
verging into independent branches (Fig. 2B). The
information resulting from the bush model is
I
bush
(R
1
, :::, R
n
; S)  =
1
2
log
2
  1   n
s
2
S
s
2
SR
   
2
wheres
2
S
  is the variance of the signal distribution,
and  s
2
SR
  is  the  noise  (variance)  introduced  in
each  branch.   Thus,   the  information  can  grow
logarithmically  with  the   number   of   branches
without an upper bound. In contrast, the informa-
tion resulting from the tree model is
I
tree
(R
1
, :::, R
n
; S)  =
1
2
log
2
  1 
  ns
2
S
=s
2
CR
1   ns
2
SC
=s
2
CR
   
  3
where  s
2
SC
  and  s
2
CR
  are the trunk and branch
noises, respectively (see SOMsection 3.3). As the
number   of   branches   increases,   the  information
asymptotically  approaches  an  upper  limit   equal
to   the   mutual   information   between   the   input
signal   and  the  common  intermediate.   Thus,   the
information lost to noise in the trunk determines
the maximum throughput of a tree network.
The  key  difference  between  bush  and  tree
networks is the absence or presence of this trunk-
based  information  bottleneck.   The  biochemical
structure of a network can resemble a tree, but if
there  is  little  loss  of   information  upstream,   the
A
B
C   D
Fig.  2.  Information gained by signaling through a network comprising mul-
tiple  communication  channels.  (A)  Schematic  of  a  bush  network  with  inde-
pendent channels lacking an information bottleneck. (B) Schematic of a tree
network  with  channels  sharing  a  common  trunk  that  forms  an  information
bottleneck. Circles represent noise introduced in the indicated portions of the
signaling network; see text for definition of symbols. (C) Comparison of bush
and tree model predictions for the capacity of the TNF network to experimental
values.   At   30  min,   the  NF-kB  and  ATF-2  pathways  together  capture  more
information about TNF concentration than either pathway alone (bars 1 to 3),
and the tree rather than bush model accurately predicts this increase (bars 3 to
5). The tree model further predicts a receptor-level bottleneck of 1.26  T 0.13
bits  (bar  6).  (D)  Joint  distribution  of  NF-kB  and  ATF-2  responses  to  30-min
stimulation   of   TNF.   Each   data   point   represents   a   single   cell,   and   each
concentration of TNF examined is shown with a distinct color.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   355
REPORTS
bush  model  lacking  a  bottleneck  might  best  es-
timate  the  capacity  of  the  network.  Additionally,
the  bush  and  tree  models  make  various  semi-
quantitative   predictions   (see   SOM  section   6),
such  as  the  information  captured  by  a  network
based  on  the  capacities  of   its  component   path-
ways. For example, for a bush network compris-
ing  two  pathways   each  with  1-bit   responses,
Eq.  2  implies  s
2
S
=s
2
SR
   3  and  that  together
they should yield
  1
2
log
2
1  23  1:4  bits.
TNF   activates   the   NF-kB  and   c-Jun   N-
terminal kinase (JNK) pathways, stimulating nu-
clear  localization  of  NF-kB  and  phosphorylated
activating transcription factor2 (ATF-2) (fig. S4),
respectively  (29).   To  determine  if  the  TNF  sig-
naling network contains an appreciable upstream
information  bottleneck  limiting  the  information
captured by these pathways, we examined wheth-
er the bush (bottleneck absent) or tree (bottleneck
present)  network  model  better  approximates  the
network (fig. S5). The models are applicable be-
cause  the  NF-kB  (Fig.  1D)  and  ATF-2  (fig.  S6)
response distributions are approximately Gaussian
at all TNF concentrations. We found that NF-kB
alone  yielded  at   most   0.92  bits  of   information
about   TNF  concentration,   and  ATF-2  alone
yielded  at  most  0.85  T  0.02  bits  (fig.  S1B  and
table S1). Together, the bush model predicts that
these pathways jointly yield 1.27 T 0.01 bits (Fig.
2C),   and  a  similar   model   assuming  indepen-
dent  pathway  responses  that  are  not  necessarily
Gaussian likewise predicts an increase to 1.13  T
0.01  bits.  The  actual  information  determined  by
dual-staining immunocytochemistry (Fig. 2D) was
1.05  T  0.02  bits,   much  lower  than  both  predic-
tions (Fig. 2C), demonstrating that the bush mod-
el  does  not  approximate  the  TNF  network  well.
In  contrast,  the  tree  model  predicts  1.03  T  0.01
bits,  matching  the  experimental  value  within  er-
ror (Fig. 2C), and also correctly predicts the sta-
tistical dependency between the responses given
the signal (fig. S7).
The correspondence between the tree mod-
el predictions and experimental measurements
strongly  indicates  that   the  network  contains  an
information  bottleneck.  The  tree  model  predicts
that   the  maximum  information  that   can  pass
through the bottleneck is 1.26 T 0.13 bits (Fig. 2C),
A   B   C   D
E
Fig.   3.   Effect  of  negative  feedback  to  the  bottleneck  on  information  transfer.   (A)  TNF  signaling  network
diagram  showing  A20-mediated  negative  feedback  to  the  information  bottleneck.  (B)  Comparison  of  infor-
mation about TNF concentration captured with and without A20 negative feedback. The information is larger at
30 min but smaller at 4 hours in wild-type cells as compared to A20
/
cells. (C and D) Schematic of NF-kB
dynamics  in  wild-type  and  A20
/
mouse  fibroblasts  exposed  to  saturating  concentrations  of  TNF.  Average
dynamics (black) and the expected magnitudes of the dynamic range (double arrow) and noise (single arrow)
are  shown. See  fig.  S9  for  experimental support.  (E)  Comparison  of  NF-kB  responses  to  zero  (basal)  or  sat-
urating concentrations of TNF. Differences in the means with and without TNF indicate the dynamic range, and
error bars (SD) indicate the noise.
A   B   C
Fig.  4. Information gained by signaling through networks of multiple genes. (A)
Plot shows the unique curve (solid black) determined by the tree model (inset),
passing through the experimentally determined values (circles), for information as
a function of the number of copies of a NF-kB reporter gene. The upper limit,
corresponding to the maximum information captured by integrating NF-kB ac-
tivity over time, is 1.64  T  0.36 bits (blue dashed line). (B) Expression-level dis-
tributions of clonal cell lines containing different numbers of copies of an NF-kB
reporter gene in response to ~10 hours of TNF exposure. (C) Time courses cor-
responding to individual cells showing cell-to-cell differences in the onset and rate
of NF-kB reporter gene expression (left). In each cell, expression is nearly linear
and deterministic in time, as quantified by the correlation coefficient (right) of the
time course after onset of expression (shown schematically in inset on left).
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 356
REPORTS
corresponding  to just  2
1.26
=  2.3  distinguishable
TNF concentrations. The known biochemistry of
TNF signaling implies that the bottleneck (trunk)
comprises the steps of TNF receptor complex ac-
tivation common to both pathways, including lig-
and binding, receptor trimerization, and complex
formation  and  activation.   Because  all   TNF  sig-
naling passes through the receptor complex, mul-
tiple   pathways   in  the   TNF  signaling  network,
activated at the 30-min time point, only modestly
increase  the  information  about   TNF  concentra-
tion regardless of the number of pathways or their
fidelity.
We next explored whether negative feedback,
which can reduce noise (12,  30,  31), might alle-
viate the receptor-level signaling bottleneck. The
information captured by a single channel (Eq. 2,
n = 1) can be written as
  1
2
log
2
s
2
R
=s
2
SR
. Thus,
negative feedback can have equivocal effects on
information, depending on the balance of the tend-
encies for negative feedback to reduce both the
dynamic range of the signaling response (32), rep-
resented  by  the  response  variance  s
2
R
,  and  noise,
represented bys
2
SR
. Indeed, comparison of wild-
type   cells   and  cells   lacking  A20  (fig.   S8),   an
inhibitor  of  TNF  receptor  complexes  whose  ex-
pression is up-regulated by NF-kB(33) (Fig. 3A),
showed that A20-mediated negative feedback in-
creases information at the 30-min time point, but
decreases it at 4 hours (Fig. 3B).
To  understand  these  different   outcomes,   we
examined  how  A20  affects  the  dynamic  range
and  noise  at  either  time  point.  At  the  early  time
point, constitutively expressed A20 inhibits basal
NF-kB  activity,   but   TNF  does  not   induce  A20
expression  rapidly  enough  to  affect  saturating
levels of NF-kB at 30 min (Fig. 3, C and D, and
fig. S9) (17,  34). Hence, A20 negative feedback
decreases  noise,   primarily  at   low  TNF  concen-
trations, and also increases the dynamic range by
lowering  basal   NF-kB  levels  (Fig.   3E  and  fig.
S10A), explaining why information at 30 min is
higher for wild-type than for A20
/
cells (Fig. 3B).
In  contrast,   at   the   late   time   point,   A20  is   in-
creased in wild-type cells (17,  34). The negative
feedback  decreases  noise  at  all  TNF  concentra-
tions  but   also  decreases  the  dynamic  range  by
strongly  suppressing  the  maximum  inducible
NF-kB activity (Fig. 3E and fig. S10A). The net
effect  is  lower  information  for  wild-type  versus
A20
/
cells at 4 hours (Fig. 3B).
We observed that A20 negative feedback sim-
ilarly both improves and limits information at the
early and late time points, respectively, for ATF-2
alone, or together with NF-kB (Fig. 3B and fig.
S10B), consistent with A20 affecting the portion
of the network common to both pathways. Nev-
ertheless, the maximal information about TNF con-
centration acquired with or without A20-mediated
negative  feedback  was  still  ~1  bit,   suggesting
limited advantages for mitigating the information
bottleneck  in  this  pathway  by  using  negative
feedback.
We  next  considered  whether  networks  com-
prising  multiple  target   genes  can  capture  sub-
stantial   amounts   of   information  through  time
integration.  If  the  target  gene product  lifetime is
long compared to its transcription and translation
time  scales,   the  accumulated  protein  concentra-
tion is approximately proportional to the time in-
tegral of signaling activity, thereby averaging out
temporal fluctuations (35, 36). However, the bio-
chemical  readout  of  protein  synthesis  can  intro-
duce  extra  noise,   confounding  determination  of
the  information  contained  in  the  time  integral.
Fortunately,  the  maximum  information  captured
by  a  tree  network,  in  which  the  time  integral  of
transcription factor activity is the intermediate sig-
nal  activating  multiple  independent  target  genes
(Fig. 4A, inset), is determined by the trunk (time
integration) rather than branch noise (readout mech-
anism).   We  measured  the  information  captured
by such  tree  networks  in cells  stably  transfected
with different copy numbers (1.8-fold difference,
as  determined  by  polymerase  chain  reaction)  of
the  gene  coding  for   a  stable  green  fluorescent
protein  (GFP)  (37)  reporting  on  NF-kB  activity
(Fig. 4B). Using the tree model to extrapolate the
extent   of   the  bottleneck,   under   the  assumption
that ~10 hours of TNF exposure induces similar
expression  level   and  noise   for   each  gene,   in-
dicates that 1.64  T  0.36 bits is the maximum  in-
formation  that   integrating  NF-kB  activity  over
the   experimental   time   period   can   yield   about
TNF  concentration  (Fig.   4A),   regardless  of   the
readout mechanism.
To understand why information was only mod-
erately  higher  compared  to  a  single  time  point
(1.64  versus  0.92  bits),   we  monitored  GFP  re-
porter gene expression in individual cells, finding
that, for any given cell, GFP accumulated linearly
in time in a nearly deterministic fashion, although
its onset and accumulation rate varied fromcell to
cell   (Fig.   4C).   This  is  consistent   with  observa-
tions made with live cell probes (1820) showing
NF-kB  dynamics  to  be  essentially  deterministic
over the experimental time scale within each cell,
but   distinct   across  cells.   We  thus  conclude  that
the  ability  of time  integration  to  increase  the  in-
formation about TNF concentration is limited by
the lack of rapid temporal fluctuations that would
otherwise  be  suppressed  by  integration  over  the
10-hour response.
Finally, we considered signaling via multiple
cells,  each  considered  as  separate  information
channels  within  a  network  (Fig.   5A,   inset).   An
ensemble  of   cells  resembles  a  bush  network  if
each cell directly and independently accesses the
same  signal,  and  because  bush  networks  do  not
contain  trunk-based  bottlenecks,   substantial   in-
creases in information might be obtained. To test
this  hypothesis,  we  analyzed  the  collective  TNF
response  of  different   numbers  of  cells,   as  mea-
sured  by  immunocytochemistry.   We  varied  cell
number  by  considering  cells  within  nonoverlap-
ping  circular   regions  of   variable  diameter   (Fig.
5B) and used the average NF-kB response with-
in each region to simulate cells contributing to a
collective  response  in proportion  to their  NF-kB
activity.   The  bush  model  predicts  (Eq.  2),  and
the  data  confirm  (Fig.  5A),  that  the  information
should increase logarithmically with the number
of   independently  signaling  cells   functioning
collectively.
Moreover, we found that networks of just 14
cells  can  yield  up  to  1.8  bits  of  information,  far
greater   than  the  other   network  types   analyzed
above. Because ensembles of this size can plau-
sibly experience a similar concentration of a dif-
fusing signal such as TNF and function collectively
(21,   38)   [e.g.,   TNF-activated  blood  vessel   en-
dothelial  cells (39)],  collective cell  behavior  can
effectively  increase  the  information  gained  and
produce  responses   that   can  discriminate  be-
tween  many  TNF  concentrations.   Nonetheless,
networks relying on cell-cell communication can
still  contain  bottlenecks.   For  instance,   TNF  can
be  secreted  by  macrophages  stimulated  by  lipo-
polysaccharide   (LPS)   from  invading   bacteria,
with  the  information  about  the  initial  LPS  dose
lost   within  the  macrophage  signaling  networks
before secretion of TNF.
By treating biochemical signaling systems as
information  theoretic  communication  channels,
we have rigorously and quantitatively shown that,
Fig.   5.   Information  gained  by  signaling  through  networks  of   multiple  cells.   (A)   Comparison  of   ex-
perimentally measured information obtained by collective cell responses (circles) versus logarithmic trend
(solid  black  line)   predicted  the  bush  model   (inset).   (B)   Schematic  of   methodology  used  to  measure
collective cell responses.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   357
REPORTS
in a single cell, noise can substantially restrict the
amount   of   information  transduced  about   input
intensity,  particularly  within  individual  signaling
pathways.   The  bush  and  tree  network  models,
which provide a unified theoretical framework for
analyzing branched motifs widespread in natural
and   synthetic   signaling   networks,   further   dem-
onstrated  that   signaling  networks  can  be  more
effective  in  information  transfer,   although  bot-
tlenecks  can  also  severely  limit  the  information
gained. Receptor-level bottlenecks restrict the TNF
and also PDGF signaling networks (fig. S11) and
may be prevalent in other signaling systems.
We   explored   several   strategies   that   a   cell
might use to overcome restrictions due to noise.
We  found  that   negative  feedback  can  suppress
bottleneck noise, which can be offset by concom-
itantly  reduced  dynamic  range  of  the  response.
Time   integration   can  increase   the   information
transferred, to the extent that the response under-
goes substantial dynamic fluctuations in a single
cell over the physiologically relevant time course.
The  advantage  of   collective  cell   responses  can
also be substantial, but limited by the number of
cells  exposed  to  the  same  signal   or   by  the  in-
formation present in the initiating signal itself.
Responses incorporating the signaling history
of   the  cell   might   also  increase  the  information
(40,   41).   For  instance,   responses  relative  to  the
basal  state  (fold-change  response)  might  be  less
susceptible  to  noise  arising  from  diverse  initial
states   (23),   although  this   does   not   necessarily
translate  into  large  amounts  of  transferred  infor-
mation (table S1). Similarly, for the reporter gene
system described here (fig. S12), ~0.5 bits of ad-
ditional information can be obtained if a cell can
determine expression levels at both early and late
time  points.   However,   noise  in  the  biochemical
networks that a cell uses to record earlier output
levels   and  to  later   compute  the  final   response
may nullify the information gain potentially pro-
vided by this strategy. Overall, we anticipate that
the  information  theory  paradigm  can  extend  to
the   analysis   of   noise-mitigation   strategies   and
information-transfer   mechanisms   beyond  those
explored here, in order to determine what specific
signaling systems can do reliably despite noise.
References  and  Notes
1.   J. G. Albeck, J. M. Burke, S. L. Spencer, D. A. Lauffenburger,
P. K. Sorger, PLoS Biol. 6, e299 (2008).
2.   N.   Rosenfeld,   J.   W.   Young,  U.   Alon,   P.   S.   Swain,
M.   B.   Elowitz,   Science  307,  1962  (2005).
3.   T.   J.   Perkins,   P.   S.  Swain,   Mol.   Syst.   Biol.   5,   326
(2009).
4.   W.   J.   Blake,  M.   Kaern,   C.   R.   Cantor,   J.   J.   Collins,   Nature
422,  633  (2003).
5.   M.   B.   Elowitz,   A.   J.   Levine,   E.   D.   Siggia,   P.   S.   Swain,
Science  297,  1183  (2002).
6.   J.   Paulsson,   Nature  427,   415  (2004).
7.   J.   M.   Pedraza,   A.   van  Oudenaarden,   Science  307,
1965  (2005).
8.   J.   M.   Raser,   E.   K.   OShea,   Science  304,   1811
(2004).
9.   T. M. Cover, J. A. Thomas, Elements of Information Theory
(Wiley,   New  York,   1991).
10.   R. R. de Ruyter van Steveninck, G. D. Lewen, S. P. Strong,
R.   Koberle,   W.   Bialek,   Science  275,   1805  (1997).
11.   D.   Fuller  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.  107,  9656
(2010).
12.   E.   Ziv,   I.   Nemenman,   C.   H.   Wiggins,   PLoS  ONE  2,
e1077  (2007).
13.   G.   Tkacik,   C.   G.  Callan  Jr.,   W.   Bialek,   Proc.   Natl.   Acad.
Sci.   U.S.A.   105,  12265  (2008).
14.   P. Mehta, S. Goyal, T. Long, B. L. Bassler, N. S. Wingreen,
Mol.   Syst.   Biol.   5,   325  (2009).
15.   R. Cheong, A. Hoffmann, A. Levchenko, Mol. Syst. Biol. 4,
192  (2008).
16.   R.  Cheong, C.  J. Wang, A.  Levchenko,  Mol.  Cell.  Proteomics
8,  433  (2009).
17.   S.   L.   Werner  et  al.,   Genes  Dev.   22,  2093  (2008).
18.   S.   Tay  et  al.,   Nature  466,  267  (2010).
19.   L.   Ashall   et  al.,   Science  324,   242  (2009).
20.   D.   E.   Nelson  et  al.,   Science  306,  704  (2004).
21.   R.   Cheong  et  al.,   J.   Biol.   Chem.   281,  2945  (2006).
22.   A.   Hoffmann,   A.   Levchenko,   M.   L.   Scott,   D.   Baltimore,
Science  298,   1241  (2002).
23.   C.  Cohen-Saidon,  A.  A.  Cohen,  A.  Sigal,  Y.  Liron,  U.  Alon,
Mol.   Cell   36,  885  (2009).
24.   X.   R.   Bao,   I.   D.   Fraser,   E.  A.   Wall,   S.  R.   Quake,
M.   I.   Simon,   Biophys.   J.   99,  2414  (2010).
25.   M.   Coppey,  A.   N.   Boettiger,   A.   M.   Berezhkovskii,
S.   Y.   Shvartsman,  Curr.   Biol.   18,  915  (2008).
26.   B.   B.  Averbeck,  P.   E.   Latham,   A.   Pouget,
Nat.   Rev.   Neurosci.   7,   358  (2006).
27.   J.   W.   Pillow  et  al.,   Nature  454,   995  (2008).
28.   E.  Schneidman,  W.  Bialek,  M.  J.  Berry  II,  J.  Neurosci.  23,
11539  (2003).
29.   H. Wajant, K. Pfizenmaier, P. Scheurich, Cell Death Differ.
10,  45  (2003).
30.   A.   Becskei,   L.   Serrano,   Nature  405,   590  (2000).
31.   I.   Lestas,   G.   Vinnicombe,  J.   Paulsson,   Nature  467,
174  (2010).
32.   R.   C.   Yu  et  al.,   Nature  456,   755  (2008).
33.   I.   E.   Wertz  et  al.,   Nature  430,  694  (2004).
34.   E.   G.  Lee  et  al.,   Science  289,   2350  (2000).
35.   V.   Shahrezaei,   P.   S.   Swain,   Proc.   Natl.   Acad.   Sci.   U.S.A.
105,   17256  (2008).
36.   S.   Krishna,   M.   H.   Jensen,   K.   Sneppen,  Proc.   Natl.   Acad.
Sci.   U.S.A.  103,  10840  (2006).
37.   S.   Thierfelder,   K.   Ostermann,   A.   Gbel,  G.   Rdel,
Appl.   Biochem.   Biotechnol.   163,  954  (2011).
38.   K. Francis, B. O. Palsson, Proc. Natl. Acad. Sci. U.S.A. 94,
12258  (1997).
39.   J.   Parkin,   B.   Cohen,   Lancet  357,  1777  (2001).
40.   I.   Nemenman,   G.  D.   Lewen,   W.   Bialek,   R.   R.   de  Ruyter
van  Steveninck,   PLOS  Comput.   Biol.   4,   e1000025
(2008).
41.   S.  P.   Strong,   R.  Koberle,   R.   R.  de  Ruyter  van  Steveninck,
W.   Bialek,   Phys.   Rev.   Lett.   80,  197  (1998).
Acknowledgments:   We  thank  A.   Hoffmann,   M.   Simon,
S.  Shvartsman,  C.  Cohen-Saidon,  and  U.  Alon  for  sharing
data  and  materials;   A.   Ganesan  and  H.   Chang  for
experimental   assistance;   and  P.   Iglesias,   Y.   Qi,  and
A.   Feinberg  for  insightful   discussions  and  reviewing
drafts  of  the  manuscript.   This  work  was  supported  by
NIH  grants  GM072024 and  RR020839  (R.C.,  A.R.,  C.J.W.,
and  A.L.)  and  CA132629  (I.N.),   the  Medical   Scientist
Training  Program  at  the  Johns  Hopkins  University  (R.C.),
and,   in  early  stages  of  the  work,   the  Los  Alamos
National   Laboratory  Directed  Research  and  Development
program  (I.N.).
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1204553/DC1
Materials  and  Methods
SOM  Text
Figs.   S1  to  S12
Table  S1
References  (4255)
18  February  2011;   accepted  7  September  2011
Published  online  15  September  2011;
10.1126/science.1204553
ER  Tubules  Mark  Sites  of
Mitochondrial  Division
Jonathan  R.  Friedman,
1
Laura  L.  Lackner,
2
Matthew  West,
1
Jared  R.  DiBenedetto,
1
Jodi  Nunnari,
2
Gia  K.  Voeltz
1
*
Mitochondrial  structure  and  distribution  are  regulated  by  division  and  fusion  events.
Mitochondrial  division  is  regulated  by  Dnm1/Drp1,  a  dynamin-related  protein  that  forms
helices  around  mitochondria  to  mediate  fission.  Little  is  known  about  what  determines  sites
of  mitochondrial  fission  within  the  mitochondrial  network.  The  endoplasmic  reticulum  (ER)
and  mitochondria  exhibit  tightly  coupled  dynamics  and  have  extensive  contacts.  We  tested
whether  ER  plays  a  role  in  mitochondrial  division.  We  found  that  mitochondrial  division  occurred
at  positions  where  ER  tubules  contacted  mitochondria  and  mediated  constriction  before  Drp1
recruitment.  Thus,  ER  tubules  may  play  an  active  role  in  defining  the  position  of  mitochondrial
division  sites.
R
egulation of mitochondrial division is crit-
ical to normal cellular function; excess
division  is  linked  to  numerous  diseases,
including neurodegeneration and diabetes (1,  2).
The central player in mitochondrial division is
the highly conserved dynamin-related protein
(Drp1 in mammals, Dnm1 in yeast), which belongs
to  a family  of  large  guanosine  triphosphatases
(GTPases) that self-assemble to regulate mem-
brane structure (3). Division dynamins are likely
to work by oligomerizing in a GTP-dependent
manner into helices that wrap around mitochon-
dria; locally controlled assembly-stimulated GTP
hydrolysis  is  thought   to  provide  the  mechano-
chemical force that completes fission of the out-
er and inner membranes (4). There are additional
proteins required for mitochondrial division, such
as the outer membrane protein Mff (mitochondrial
fission  factor),   which  is  present   only  in  mam-
mals (5). Although general mechanisms exist for
1
Department of Molecular, Cellular, and Developmental Biol-
ogy,   University  of   Colorado,   Boulder,   CO  80309,   USA.
  2
De-
partment   of   Molecular   and   Cellular   Biology,   University   of
California, Davis, CA 95616, USA.
*To   whom  correspondence   should  be   addressed.   E-mail:
gia.voeltz@colorado.edu
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 358
REPORTS
Fig.  1.  Mitochondrial constriction and division oc-
curs at ER-mitochondrial contacts in yeast. (A) The
3D  models (left  images) of ER (green) and mito-
chondria (purple) at contact domains were imaged
by EM and tomography of high-pressure frozen yeast
cells. Middle images are 2D tomographs of contact
sites (second column, ER drawn in green) and the
corresponding 3D models of each (third column).
Contact, marked in red, is defined as regions where
the ER membrane comes within 30 nm of the mito-
chondrial  membrane,  and  ribosomes  are  excluded
(third  column).   Right   schematics  demonstrate  the
percentage of the mitochondrial circumference that
makes contact with the ER membrane [red is contact,
white is not (19)]. The diameter of each mitochon-
drion  at  positions  of  ER  contact  is  shown.  Regions
where  the  mitochondria  are  constricted  (models  a
and c) have a high percent of ER wrapping. Addi-
tional EM tomographs and analysis of constrictions
are shown in fig. S1, A and B. (B) Time-lapse images
of yeast cells expressing mito-dsRed and GFP-HDEL
(ER). A single focal plane is shown. Arrows and arrow-
heads indicate sites of mitochondrial division. A cor-
responding z-series is shown in fig. S1C. Scale bars
indicate, in (A), 200 nm; (B), 2  mm.
A
0s   40s   80s   120s   160s   200s   240s   280s
B
G
F
P
-
H
D
E
L
m
i
t
o
-
d
s
R
E
D
m
i
t
o
-
d
s
R
E
D
74%
138 nm
43%
215 nm
91%
146 nm
11%
193 nm
a
b
a
b
a
b
c
d
c
d
c
d
a
b
c
d
GFP-Sec61
mito-dsRed
mito-dsRed
A   B
GFP-Sec61
mito-dsRed
0s   10s   20s   30s   0s   10s   20s   30s
0s   10s   20s   40s
C
  0s   10s   20s   30s
D
mito-dsRed
Fig.   2.  Mitochondrial   division  occurs   at   ER-mitochondrial   contact   sites   in
mammalian cells. (A to D) Four examples of mitochondrial division over time
courses  shown  in  Cos-7  cells  expressing  GFP-Sec61b  (ER)   and  mito-dsRed.
The site of mitochondrial division (white arrows) and the position of the newly
formed mitochondrial ends (yellow arrows) are shown. Additional examples are
included  in  fig. S2A. Scale bars, 1  mm.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   359
REPORTS
recruiting Dnm1 or Drp1 to mitochondria, it is not
known  whether  there  are  specific  sites  on  mito-
chondria  that   are  marked  for   division  (6).   Fur-
thermore, both Dnm1 and Drp1 oligomerize into
helices that are much smaller than the diameter of
mitochondria (Dnm1 helices have reported mean
diameters of 109 nmin yeast and 129 nmin vitro),
suggesting  that  Dnm1  (Drp1)independent  mito-
chondrial constriction may be needed to facilitate
mitochondrial division (4,  69).
Contact sites exist between mitochondria and
the  endoplasmic  reticulum  (ER)  and  are  impor-
tant for phospholipid synthesis and calciumsignal-
ing  [for  review,  see  (10)].  Based  on  recent  data,
there are likely several types of molecular bridges
that mediate these contacts, such as the ERMES
complex identified in yeast and the mitochondrial
fusion protein mitofusin 2 (Mfn2) in mammalian
cells  (11,   12).   These  physical   contacts  are  per-
sistent and maintained under dynamic conditions
(13), suggesting that the ER-mitochondrial inter-
face is vital for function. We have used electron
microscopy (EM) and tomography to analyze the
three-dimensional   (3D)   structure  of   contacts   be-
tween  the  ER  and  mitochondria  in  the  yeast
Saccharomyces cerevisiae. We observed the high-
resolution  (~4  nm)  structure  and  3D  models  of
four  ER-mitochondrial  contacts  taken  from  two
cells  (Fig.   1A).   In  these  examples,   the  ER  was
wrapped around mitochondria to varying degrees.
In two of the four examples, the ER almost com-
pletely  circumscribed  the  mitochondrial   outer
membrane, and mitochondria were constricted at
the point of contact (mitochondrial diameter 138
nm  and  146  nm  circumscribed  versus  215  nm
and 193 nmuncircumscribed at ERcontact) (Fig.
1A;  fig.   S1,   A  and  B;  and  movies  S1  and  S2).
These  data  suggest   that   ER  tubules  associate
with  and  may  mediate  mitochondrial  constric-
tion sites.
We  thus  examined  the  role  of   ER  in  mito-
chondrial division by using fluorescence micros-
copy  in  live  yeast  cells  transformed  with  an  ER
marker  (GFP-HDEL)  and  mito-dsRed  to  image
the  behavior   of   ER  and  mitochondria  simulta-
neously  over   time.   The  vast   majority  of   mito-
chondrial division events were spatially linked to
sites of ER-mitochondrial contact (87%,  n = 112
Linescan BFP-KDEL
mito-EGFP mito-EGFP
mCherry-Drp1
BFP-KDEL
mito-EGFP
mCherry-Drp1
mito-EGFP
E
Distance (pixels)
R
e
l
a
t
i
v
e
 
f
l
u
o
r
e
s
c
e
n
c
e
i
n
t
e
n
s
i
t
y
B
D
mCherry-Drp1
GFP-Sec61
mito-BFP
mito-BFP / mCherry-Drp1 / GFP-Sec61
0s   40s   80s   120s
0s   40s   80s   120s
Always
Part of time
Never
P
e
r
c
e
n
t
 
o
f
 
p
u
n
c
t
a
e
n=101
0s   40s   80s   120s
Distance (pixels)
R
e
l
a
t
i
v
e
 
f
l
u
o
r
e
s
c
e
n
c
e
i
n
t
e
n
s
i
t
y
Distance (pixels) R
e
l
a
t
i
v
e
 
f
l
u
o
r
e
s
c
e
n
c
e
i
n
t
e
n
s
i
t
y
Drp1 localization to
ER-mitochondrial contacts
GFP-HDEL mito-CFP
Dnm1-
mCherry   Merge
A
0s
10s
20s
30s
C
Fig.  3.  Dnm1- and Drp1-mediated mitochondrial division occurs at ER con-
tact sites. (A) Time-lapse images of wild-type yeast cells expressing mito-CFP,
GFP-HDEL (ER), and Dnm1-mCherry. A single focal plane is shown. Arrows indi-
cate the site of mitochondrial division, which is marked by both ER-mitochondria
contact and Dnm1. (B) Merged image of a live Cos-7 cell expressing GFP-Sec61b
(ER), mito-BFP, and mCherry-Drp1. (C) Examples of cells as in (B) that show that
Drp1 punctae maintain colocalization with positions of ER-mitochondrial contact
over time. White arrows indicate Drp1 punctae that maintain contact with both
the ER and mitochondria. Yellow arrows indicate a rare example of Drp1 that
does not contact the ER. (D) The percentage of mitochondrial Drp1 punctae that
colocalize  with  the  ER  membrane  over  a  2-min  time  course.  (E)  Examples  of
mitochondrial constrictions at ER contact sites marked by Drp1. Left-hand im-
ages showCos-7 cells expressing mito-EGFP, BFP-KDEL (ER), and mCherry-Drp1,
merged as indicated. Right graphs are line scans drawn through the mitochon-
dria and show the relative fluorescence intensity of mitochondria (green), ER
(blue), and Drp1 (red) along its length. White arrows at constrictions on images
correspond  to  black  arrows  shown  on  the  line  scan.  Additional  examples  are
shown in fig. S4. Scale bars for (A), (C), and (E), 1  mm; (B), 5  mm.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 360
REPORTS
from  281  cells)  (Fig.  1B).  ER  tubules  crossed
over (Fig. 1B, yellow arrows) and wrapped around
mitochondria (Fig. 1B, white arrows, and  fig.
S1C). At ER-mitochondrial contact sites, mito-
chondrial constriction followed by mitochondrial
division was observed (Fig. 1B).
We  next   tested  whether   ER  plays  a  similar
role in mammalian mitochondrial division by using
fluorescence microscopy of live Cos-7 cells tran-
siently  transfected  with  fluorescent   markers  for
ER(GFP-Sec61b) and mitochondria (mito-dsRed).
We  imaged  regions  of  the  cell  periphery  where
contacts between the mitochondria and ER were
well   resolved  and  observed  that   mitochondrial
division  events  predominantly  occurred  at   sites
of contact between ERand mitochondria (94%,
n = 32 from23 cells) (Fig. 2, fig. S2A, and movies
S3 and S4). Furthermore, the majority of  events
(88%) were sites of ER tubules crossing over the
mitochondria, suggesting that the structural con-
text of the interaction is important. The frequency
of ER-associated mitochondrial division is much
higher than would be predicted on the basis of
the area of mitochondria covered by crossing ER
tubules as determined by colocalization of mito-
chondrial and ER markers (fig. S2B).
Thus, in both yeast and mammalian cells, ER
tubules   are  at   mitochondrial   division  sites   and
may be involved in mitochondrial constriction dur-
ing  this  process.   Next,   we  asked  whether   mito-
chondrial division occurs in yeast cells that have
substantially reduced levels of tubules because of
the  absence  of   the  membrane  shaping  proteins
Rtns and Yop1 (14,  15). By using both EM and
fluorescence microscopic analyses, we observed
that,  in  regions  of  mutant  cells  in  which  ER  tu-
bules   were  dramatically  reduced,   short   ER  tu-
bules  extended  out  of  the  massive  ER  cisternae
and associated with mitochondrial constrictions
and  division  events  (fig.  S3).  Thus,  ER  tubules
are  a  consistent   feature  of   ER  contact   at   mito-
chondrial   constrictions,   even   under   conditions
where   most   tubules   are   depleted.   Furthermore,
Rtns and Yop1 are dispensable for the biogenesis
of  the  ER  tubules  that  associate  with  mitochon-
drial division events.
To ask whether ER-associated division events
are spatially linked to the mitochondrial division
machinery, we determined the relationship of ER-
mitochondrial  contacts to the division dynamins
Dnm1 and Drp1. Dnm1 and Drp1 assemble into
punctate structures at steady state, and a subset
of  these  structures  are  found  on  mitochondria
and at  mitochondrial division  sites (6,   16,  17).
We imaged live yeast transformed with Dnm1-
mCherry, mitocyan fluorescent protein (CFP),
and GFP-HDEL (ER) and observed that a large
percentage  of   Dnm1  punctae  were  at   sites  of
mitochondrial-ER contact (46%,  n = 225). These
Dnm1 punctae could be observed at sites where
ER tubule crossover and mitochondrial division
occurred (Fig. 3A). In Cos-7 cells transiently trans-
fected  with  GFP-Sec61b  (ER),   mitoblue  flu-
orescent protein (BFP), and mCherry-Drp1, we
observed that the majority of Drp1 punctae sta-
bly  associated  with  mitochondria  and  localized
to ER-mitochondrial contacts over time (Fig. 3,
B  to  D,  and  movie  S5).  Furthermore,  a  subset
of Drp1 at these contacts was associated with a
mitochondrial  constriction  site  (78%,   excluding
punctae localized to mitochondrial tips,  n = 50).
The mitochondrial constrictions marked by Drp1
punctae  were  always  either  at  ER  tubule  cross-
overs (81%) or adjacent to them (19%) (Fig. 3E
and  fig.  S4).  Together,  the  localization  of  the
mitochondrial division dynamins in yeast and
mammalian cells to regions of ER-mitochondrial
contacts  and  the  observations  that  these  regions
are associated with constricted mitochondria and
subsequent  division  indicate  a  direct  role  of  the
ER in the process of mitochondrial division.
Mff   is  a  mammalian-specific  mitochondrial
outer  membrane  protein  required  for  mitochon-
drial   localization  of   Drp1  and  division  (5,   18).
Drp1 and Mff colocalize in punctate structures on
mitochondria,   and  Mff   punctae  persist   in  cells
where Drp1 expression is reduced by RNAi (18).
Thus,  Mff  punctae  may  mark  the  future  sites  of
mitochondrial   division  before  Drp1  recruitment
(18).   In  Cos-7  cells  transiently  transfected  with
C
BFP-KDEL
mito-dsRed
GFP-Mff BFP-KDEL
mito-dsRed mito-dsRed   mito-dsRed
GFP-Mff
Linescan
Distance (pixels)
R
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l
a
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i
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e
 
f
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e
s
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Distance (pixels)
R
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f
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y
BFP-KDEL
mito-dsRed
mito-dsRed
D
  GFP-Sec61
mito-dsRed
M
f
f
 
R
N
A
i
Linescan
R
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Distance (pixels)
Distance (pixels)
R
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f
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y
A
  BFP-KDEL
mito-dsRed
GFP-Mff
D
r
p
1
 
R
N
A
i
GAPDH
Drp1
siRNA
c
o
n
t
r
o
l
D
r
p
1
IB:
B
GAPDH
Mff
c
o
n
t
r
o
l
M
f
f
IB:
At ER tubule crossing   16 (64%)
Adjacent to ER tubule crossing   4 (16%)
Alongside ER tubule   3 (12%)
Not at ER   2 (8%)
Constrictions marked
by Mff (Drp1 RNAi)
n = 25
GFP-Sec61
Fig.  4.  The  ER  localizes  to  mitochondrial   constrictions  before  Drp1  and
Mff  recruitment.  (A)  Examples  of  mitochondrial  constrictions  at  ER  contacts
marked by Mff in Cos-7 cells depleted of Drp1. Left and center images show
these  cells  expressing  mito-dsRed,  BFP-KDEL  (ER),  and  GFP-Mff,  merged  as
indicated.  Right  graphs  are  line scans  drawn  through  the  mitochondria and
show the relative fluorescence intensity of mitochondria (red), ER (blue), and
Mff  (green)  along  their  length.  White  arrow  positions  at  constrictions  corre-
spond to black arrows on the line scan. Additional examples are shown in fig.
S6. (B)  Western  blots  with  antibody  against  Drp1  (top)  or  Mff  (bottom)  and
GAPDH demonstrate depletion of Drp1 in lysates from cells transfected with
siRNA against Drp1 [as in (A)] or Mff [as in (D)] compared with control RNAi
cells.   (C)  The  number  of  Mff-localized  mitochondrial   constrictions  in  Drp1-
depleted cells that colocalize with ER tubules, from 23 cells. (D) As in (A), for
cells depleted of Mff and expressing GFP-Sec61b (ER; green on line scan) and
mito-dsRed (red on line scan). Scale bars for (A) and (D) large left images, 5 mm;
(A) and (D) smaller center images, 1  mm.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   361
REPORTS
GFP-Mff, mCherry-Drp1, and mito-BFP, we ob-
served  that   Mff   circumscribed  and  localized  to
punctae on mitochondria, the majority of which
colocalized with Drp1 (fig. S5, A  to C). To test
whether   Mff   punctae   localize   to  ER  contacts
independently  of  Drp1,  we  depleted  Drp1  from
Cos-7 cells with small interfering RNA (siRNA)
and cotransfected these cells with GFP-Mff, mito-
dsRed,   and  BFP-KDEL  (ER).   Drp1  was  sub-
stantially  depleted  in  Drp1  RNA  interference
(RNAi)   cells   in  comparison  with  the  control
cells (Fig. 4B). Selective depletion of Drp1 was
further supported by the aberrant and elongated
mitochondrial morphology in Drp1 RNAi cells
(Fig. 4A and fig. S5D). As expected (18), in Drp1-
depleted cells, Mff punctae localized to mitochon-
dria  (Fig.   4A).   We  asked  whether   mitochondria
were constricted at Mff punctae in the absence of
Drp1,  and  if  so,  whether  these  sites  localized  to
ERcontacts. Of the 25 constrictions we resolved,
16 were at an ER crossover (64%), and another
4 were adjacent to an ER tubule crossing (16%)
(Fig. 4, Aand C, and fig. S6). Thus, Mff localizes
in  a  Drp1-independent  manner  to  mitochondrial
constrictions at sites of ERcontact. We next asked
whether the ER localizes to regions of mitochon-
drial   constriction  in  the  absence  of   Mff.   Cos-7
cells were depleted of Mff by siRNAand cotrans-
fected  with  GFP-Sec61b  (ER)  and  mito-dsRed.
As  expected,  mitochondrial  morphology  was
elongated in these cells (Fig. 4, B and D, and
fig. S5E). In cells  depleted of Mff, we observed
mitochondrial constriction at sites of ER contact,
indicating that ER-mitochondrial contacts form
and mark positions of mitochondrial constriction
independently of both Mff and Drp1 recruitment
(Fig. 4D).
Here, we have shown that ER-mitochondrial
contacts are a conserved feature of mitochondrial
division. We envision two ways that ER contact
might directly regulate mitochondrial division: (i)
ERproteins intimately participate in division, and/or
(ii) ER tubules physically wrap around and con-
strict  mitochondria  to  a  diameter  comparable  to
Dnm1 and Drp1 helices to facilitate their recruit-
ment and assembly to complete fission (fig. S9).
The latter is attractive given that the diameter of
Dnm1 helices (~110 to 130 nm) is considerably
narrower  than  that  of  mitochondria  and  is  quite
similar  to  the  diameter  of  constricted  mitochon-
dria at ER tubule contacts (138 nm and 146 nm)
(4,  69). Regardless of the exact mechanism, the
ER appears to mark the division site and is likely
to be an active participant in this process, because
it remains in contact with the mitochondria through
the entire fission event. Many human diseases are
associated with excessive mitochondrial division,
raising the intriguing possibility that these diseases
could  involve an alteration of ER-mitochondrial
contacts.
References  and  Notes
1.   D.   H.   Cho,   T.   Nakamura,   S.  A.   Lipton,   Cell.   Mol.   Life  Sci.
67,  3435  (2010).
2.   Y. Yoon, C. A. Galloway, B. S. Jhun, T. Yu, Antioxid. Redox
Signal.   14,  439  (2011).
3.   L.   L.   Lackner,   J.   M.  Nunnari,   Biochim.  Biophys.   Acta
1792,  1138  (2009).
4.   E.   Ingerman  et  al.,   J.   Cell   Biol.   170,  1021  (2005).
5.   S.  Gandre-Babbe,  A.  M.  van  der  Bliek,  Mol.  Biol.  Cell  19,
2402  (2008).
6.   A. Legesse-Miller, R. H. Massol, T. Kirchhausen,  Mol. Biol.
Cell   14,  1953  (2003).
7.   A.   M.   Labrousse,   M.   D.   Zappaterra,   D.   A.   Rube,
A.   M.   van  der  Bliek,   Mol.   Cell   4,   815  (1999).
8.   Y.   Yoon,   K.   R.   Pitts,   M.   A.   McNiven,  Mol.   Biol.   Cell   12,
2894  (2001).
9.   J.   A.   Mears  et  al.,   Nat.   Struct.   Mol.   Biol.   18,   20
(2011).
10.   O.   M.   de  Brito,   L.   Scorrano,   EMBO  J.   29,   2715
(2010).
11.   O.   M.   de  Brito,  L.   Scorrano,   Nature  456,  605
(2008).
12.   B.   Kornmann  et  al.,   Science  325,  477  (2009);   10.1126/
science.1175088.
13.   J.   R.   Friedman,   B.   M.   Webster,   D.   N.   Mastronarde,
K.   J.   Verhey,   G.   K.   Voeltz,   J.   Cell   Biol.   190,   363
(2010).
14.   M.   West,  N.   Zurek,   A.   Hoenger,   G.  K.   Voeltz,   J.  Cell   Biol.
193,   333  (2011).
15.   G.   K.   Voeltz,   W.   A.   Prinz,   Y.   Shibata,   J.   M.   Rist,
T.   A.   Rapoport,   Cell   124,   573  (2006).
16.   H.   Sesaki,   R.   E.   Jensen,   J.  Cell   Biol.   147,   699
(1999).
17.   E.   Smirnova,   L.   Griparic,   D.   L.   Shurland,
A.   M.   van  der  Bliek,   Mol.   Biol.   Cell   12,   2245
(2001).
18.   H.   Otera  et  al.,   J.   Cell   Biol.   191,  1141  (2010).
19.   Materials  and  methods  are  available  as  supporting
material   on  Science  Online.
Acknowledgments:   This  work  is  supported  by  NIH  grant
R01  GM083977  and  a  Searle  Scholar  award  (to  G.K.V.),
NIH  training  grant  GM08759  (to  J.R.F.),   NIH  grant
R01  GM062942  and  an  American  Heart  Innovative
Research  Grant  (to  J.N.),  and  grants  from  the  Biological
Sciences  Initiative  (BURST  grant)  and  the  Undergraduate
Research  Opportunity  Program  at  the  University  of
Colorado  (to  J.R.D.).   We  thank  the  Boulder  3D  Electron
Microscopy  facility  for  shared  equipment  and  helpful
suggestions.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1207385/DC1
Materials  and  Methods
SOM  Text
Figs.   S1  to  S9
References  (2029)
Movies  S1  to  S5
22  April   2011;   accepted  17  August  2011
Published  online  1  September  2011;
10.1126/science.1207385
Antimicrobial  Peptides  Keep  Insect
Endosymbionts  Under  Control
Frdric  H.  Login,
1,2
Sverine  Balmand,
1,2
Agns  Vallier,
1,2
Carole  Vincent-Mongat,
1,2
Aurlien  Vigneron,
1,2
Michle  Weiss-Gayet,
2,3
Didier  Rochat,
4
Abdelaziz  Heddi
1,2
*
Vertically  transmitted  endosymbionts  persist  for  millions  of  years  in  invertebrates  and  play  an
important  role  in  animal  evolution.  However,  the  functional  basis  underlying  the  maintenance
of  these  long-term  resident  bacteria  is  unknown.  We  report  that  the  weevil  coleoptericin-A  (ColA)
antimicrobial peptide selectively targets endosymbionts within the bacteriocytes and regulates their
growth  through  the  inhibition  of  cell  division.  Silencing  the  colA  gene  with  RNA  interference
resulted  in  a  decrease  in  size  of  the  giant  filamentous  endosymbionts,  which  escaped  from  the
bacteriocytes  and  spread  into  insect  tissues.  Although  this  family  of  peptides  is  commonly
linked  with  microbe  clearance,  this  work  shows  that  endosymbiosis  benefits  from  ColA,
suggesting  that  long-term  host-symbiont  coevolution  might  have  shaped  immune  effectors
for  symbiont  maintenance.
C
ooperative  associations  between  animals
and symbiotic bacteria are widespread in
nature and common in insects that exploit
unusually  restricted  nutritional   resources  (1).   In
manyinsects, intracellular bacteria (endosymbionts)
are  transmitted  vertically  and  provide  nutrient
supplementation   to   their   hosts,   thereby   im-
proving  their  adaptive  traits  and  their  invasive
power (24).
However, maintaining the beneficial nature of
this long-term relationship requires both the host
and  the  symbiont   to  constrain  adaptive  interac-
tions. Genomic and evolutionary data have shown
that major deletions and mutations of genes occur
in endosymbionts, some of which are involved in
bacterial virulence and host tolerance (57). Data
on  how  host   immune  systems  have  evolved  to
tolerate  cooperative  bacteria  remain  scarce  and
are  mainly  limited  to  extracellular   associations
with  environmental   and/or   horizontal   symbiont
transmission (8,  9).
To  protect  permanent  endosymbionts  from
the hosts systemic immune response, and prevent
competition  with  opportunistic  invaders,  sym-
bionts  are  sequestered  in  bacteria-bearing  host
cells, called the bacteriocytes, which, in some spe-
cies, group together to forma bacteriome (10). To
investigate  the  immune  specificities  of  bacterio-
cytes, we have studied associations with Sitophilus
1
INSA-Lyon, INRA, UMR203 BF2I, Biologie Fonctionnelle Insectes
et Interactions, F-69621Villeurbanne, France.
2
Universitde Lyon,
F-69003  Lyon,   France.
  3
Universit  Lyon  1,   CNRS  UMR5534,
Centre de Gntique et de Physiologie Molculaire et Cellulaire,
F-69622 Villeurbanne, France.
4
INRA, Universit Pierre et Marie
Curie, UMR1272 Physiologie de lInsecte Signalisation et Com-
munication, F-78026 Versailles, France.
*To   whom  correspondence   should  be   addressed.   E-mail:
abdelaziz.heddi@insa-lyon.fr
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 362
REPORTS
genus. This genus of beetle includes three cereal
pest species (Sitophilus oryzae, S. zeamais, and S.
granarius), all of which share intimate intracellular
symbiosis with a Gram-negative g-Proteobacterium,
called   Sitophilus   primary  endosymbiont   (SPE)
(11,   12).   In  contrast  to  Buchnera  in  aphids,   the
Sitophilus  association  with  SPE  is  relatively  re-
cent [dating to 20 million years ago (Ma)] (13, 14).
The  SPE  genome  has  not   suffered  appreciable
genome shrinkage (15) and retains secretion sys-
tems  and  bacterial   wall   elements  that   are  impli-
cated in bacterial recognition by the host immune
receptors  (6).   Transcriptomic  data  revealed  that
SPE induces a strong systemic response when in-
jected into weevil hemolymph (16), whereas per-
manent infection of bacteriocytes with SPE leads
to  the  up-regulation  of   only  one  antimicrobial
peptideencoding   gene   coleoptericin-A  (colA,
fig. S1) (16).
In  immunohistochemistry  experiments   with
antibody against ColA (14), we found that, in apo-
symbiotic insects,  colA is expressed constitutively
in epithelial cells surrounding the intestine and in
the fat body, with a high concentration under the
cuticle (Fig. 1Band fig. S2). In symbiotic insects,
colAis further expressed in all the tissues housing
endosymbionts (Fig. 1B). Similarly, follicular cells
also  expressed  ColA  as  a  thin  layer  around  the
oocytes, and ColA signals were stronger in bacte-
riocytes surrounding bacteriomes (Fig. 1B). Thus,
a relatively high expression of colAin tissues facing
the external environment, and at the boundary of
tissues housing endosymbionts, supports the idea
that  ColA  may  either prevent  pathogen intrusion
or   retain  endosymbionts   within  the  bacteriomes
and oocytes. Moreover, ColA appeared to colocal-
ize with endosymbionts in bacteriocytes (Fig. 1B).
Using immunogold electron microscopy, we found
ColA located inside SPE cytoplasm (Fig. 1C), and
some ColAspots were also attached to the bacterial
membrane surface.  Overall, microscopic observa-
tions indicate that ColA expression targets endo-
symbionts in both somatic and germ cell lines.
We  tested  the  antimicrobial  activity  of  ColA
against microbes. The weevil paralog ColB was
used   for   comparison   because   the   colB  gene,
unlike  colA,   is  down-regulated  in  bacteriocytes
(16) and ColBshows important sequence identity
with  ColA  (fig.   S3).   ColA  and  ColB  showed
similar  bactericidal  activity  against  the  Gram-
positive   Micrococcus   luteus   and   the   Gram-
Fig.   1.   ColA peptide distribution in weevil tis-
sues.  (A)  Schemes  of  larva  and  adult  weevils
showing bacteriome localizations (in red). (B) (Up-
per panel) Tissues from aposymbiotic S. zeamais:
Left and middle images are cuticle sections stained
with a preimmune serum [negative controls can
be found in SOM (14)] and with antibody against
ColA (anti-ColA), respectively; the right image
is a gut section stained with anti-ColA. ColA
signals are detected in the fat body, with relatively high intensity under the cuticle and within gut epithelial cells. (Middle and lower panels) Tissues from
symbiotic  insects  stained  with  anti-ColA.  Middle  panel:  ColA  signals  can  be  seen  in  oocytes  and  follicular  cells  (left),  in  apical  bacteriomes  of  ovaries
(middle),  and in adult mesenteric caeca  (right); lower  panel: ColA  signals in larval bacteriome  (left), within  bacteriocytes  (middle),  and in bacteriome
squashes (right) (14). Arrows indicate high ColA signals at the periphery of tissues and show ColA colocalizing with SPE in bacteriocytes and bacteriome
squashes. (C). Immunogold staining of SPE with anti-ColA. Bacteriocyte sections are shown with ColA spots inside symbiont cytoplasm and attached to
bacterial membranes.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   363
REPORTS
negative  Escherichia  coli   (Fig.   2),   whereas  the
yeast   Saccharomyces   cerevisiae   tolerated  both
peptides   (table   S1).   Both  peptides   exhibited  a
wide range of bacteriostatic activity against Gram-
negative bacteria. SPE persists in the bacteriocyte
because  colA expression may lead either to bac-
terial growth inhibition or dose-dependent bacte-
rial clearance. At bacteriostatic concentrations,
both coleoptericins halt  E.   coli growth, but  only
ColA  inhibited  cell  division  or  caused  bacterial
gigantism (Fig. 2B). The shape of  M.  luteus was
not affected by ColA or by ColB (fig. S4). Thus,
ColA and ColB have distinct functions in weevil
immunity and symbiosis in regard to their general
effect on Gram-negative bacteria.
Since the discovery of coleoptericins (17, 18),
their  function  in  the  immune  system  and  their
role  in  symbiosis  have  not  yet  been  explored.
One  notable  observation  is  that  all  the  coleop-
teran endosymbionts observed exhibit a similar
elongated  morphology  (Fig.   2C),   resembling
symbionts in other associations. For example, in
Rhizobium-legume symbiosis,  Rhizobium elon-
gation  has  been  interpreted  to  be  the  result  of
repeated  chromosome  DNA  replication  without
cell   cytokinesis  (19).   We  measured  the  relation
between  bacterial   size  and  genome  amplifica-
tion  in  E.  coli, SPE, and  Nardonella, the ances-
tral endosymbiont of weevils (125 Ma) (13). All
bacteria  were  polyploid,   and  bacterial   size  was
highly correlated with chromosome number. The
highest scores were seen in Nardonella, with 120
chromosomes observed in a giant cell of 200  mm
(Fig. 2D). Bacterial division in plants is inhibited
by nodule-specific cysteine-rich peptides (20) that
induce irreversible elongation of bacteria and ren-
der   them  incapable  of   multiplying  in  vitro.   By
using phylogenetically unrelated molecules, plants
and  animals  target   bacterial   cytokinesis  while
preserving DNA replication, hence  domesticat-
ing the bacteria as symbionts.
To  elucidate  the  mechanism  by  which  ColA
reaches  the  bacterial   cytoplasm  and  elicits  cell
elongation, we used far-Western blotting to iden-
tify  bacterial  molecules  targeted  by  ColA  and
ColB peptides. ColA specifically interacted with
OmpA,   OmpC,   rp-L2,   EF-Ts,   and  GroEL  (fig.
S5  and  table  S2).  No  interaction  was  detected
with Hsp60,  the  eukaryotic  cytosolic  homolog
of GroEL. ColB interacted with OmpC and pro-
teins involved in translation, but not with OmpA
or GroEL.
As with colicins and phages (21),  it  is likely
that Omps are receptors that allow ColA to enter
the  cell.   Tight  attachments  of  ColA  to  the  SPE
membrane (Fig. 1C) support this assumption, and
SPE genome sequence analysis showed that SPE
encodes  a  functional  ompC  gene  (table  S3).  Al-
though the genome sequence is not available, we
found  that  ColA  targets  Nardonella  of  the  palm
weevil  Rhynchophorus  ferrugineus (fig. S6), sug-
gesting that ColA may have a broad impact on
weevil symbioses. Whether  Nardonella has re-
tained omps or whether ColAenters the bacterium
by other mechanisms remains to be determined.
We propose that after entering the cytoplasm,
ColA  elicits  cell   elongation  through  interaction
with GroEL, because ColA, but not ColB, inter-
acts with GroEL protein, and because  groEL mu-
tations in  E.  coli also trigger cell gigantism (22).
The absence of any interaction between ColB and
GroELalso indicates that ColAmay have evolved
a  specific  interaction  with  GroEL.  In  this  con-
text, it is notable that GroEL is the most abundant
protein  in  insect   endosymbionts  (23);   however,
selective  up-regulation  of  groEL  has  often  been
interpreted as an adaptive mechanism for protein
folding in  endosymbionts with  a high  A+T  bias
in the genome (24).
We used RNA interference (RNAi) to inhibit
colA transcription in the larval weevils. Injection
of  dsRNAcolA  resulted  in  a  significant   reduc-
tion in the number of bacteriocyte colA transcripts
and abundance of ColA peptide for  more than 2
weeks (fig. S7). In contrast to the plant-Rhizobium
interaction,   colA  inhibition  resulted  in  the  SPE
population declining by half (Fig. 3A). However,
whether this was due to resumption of cytokinesis
or multiplication of small bacteria is unclear. We
Fig. 2. ColA and ColB activities against bacteria. (A) ColA (solid line) and ColB (dashed line) activities
against   E.   coli   (triangles)   and  M.   luteus   (squares).   ColA  and  ColB  have  a  similar   inhibitory  effect
(analysis of variance, P =0.76). They show bactericidal activities against M. luteus at low concentrations.
For  E.  coli, low concentrations of ColA and ColB have bacteriostatic activity, and higher concentrations
kill  this  bacterium.   (B)  Effect  of  low  concentrations  of  ColA  and  ColB  on  E.   coli   morphology.  Bacteria
were incubated in LB broth (left, control), in LB with 8  mM ColA (middle), or in LB with 8  mM ColB (right).
Cell  gigantism  is  observed  with  ColA  peptide  only.  (C)  Gram  staining  of  endosymbionts  from  S.  oryzae
(rod-shaped, left),  S.  zeamais  (spiral,  middle),  and  R.  ferrugineus (filamentous,  right).  (D)  Chromosome
visualization  of   E.   coli   treated  with  8  mM  ColA  (left),   SPE  (middle),   and  Nardonella  (right).   SPE  and
Nardonella  were  isolated  from  larval   bacteriomes  of   S.   oryzae  and  R.   ferrugineus,   respectively.   Chro-
mosome  number  was  highest  in  Nardonella.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 364
REPORTS
quantified SPE DNA by quantitative polymerase
chain  reaction  (qPCR)  and  showed  that   colA  in-
hibition   did   not   affect   bacterial   chromosome
replication (fig. S8). This, and the decreased num-
ber of large-sized cells after RNAi treatment (Fig.
3A), supports the former hypothesis (i.e., resump-
tion of cytokinesis and loss of the elongated form)
but  does  not  exclude  the  latter  (multiplication  of
the small-sized cells) if we consider bacterial turn-
over and de novo synthesis processes.
To  understand  ColA  function  in  symbiosis,
we  monitored  SPE  in  insects  by  fluorescence
in  situ  hybridization  (FISH)   after   dsRNA-colA
injections. Unexpectedly, several SPE cells exited
the  bacteriome  on  the  ninth  day  after  treatment
(Fig. 3B). This phenomenon increased at day 14,
when bacteria were found spread throughout the
larval   tissues.   Nevertheless,   symbiont   escape
from the bacteriome did not affect insect mortal-
ity under laboratory conditions (table S4), although
these  data  indicate  that   ColA  acts  to  prevent
bacterial tissue invasion.
The  weevil  ColA  peptide  demonstrates  sev-
eral  properties  important  to  immunity  and  sym-
biosis. It appears to act as a first line of defense in
insects against microbial intrusion, and the range
of   bacteriostatic   and   bactericidal   activities   of
ColA suggests its precise regulation of endosym-
biont   number   and  location.   The   interaction  of
GroEL  with  ColA  (but  not  with  ColB)  supports
the idea that long-term coevolution may have se-
lected ColA for this symbiotic function.
References  and  Notes
1.   N.   A.   Moran,   Curr.   Biol.   16,  R866  (2006).
2.   A.   E.  Douglas,   Annu.   Rev.   Entomol.   43,  17  (1998).
3.   A.   Heddi,   A.   M.  Grenier,   C.  Khatchadourian,   H.   Charles,
P. Nardon, Proc. Natl. Acad. Sci. U.S.A. 96, 6814 (1999).
4.   A.   G.   Himler  et  al.,   Science  332,   254  (2011).
5.   S.  Shigenobu,   H.   Watanabe,   M.  Hattori,   Y.   Sakaki,
H.   Ishikawa,   Nature  407,  81  (2000).
6.   C. Dale, G. R. Plague, B. Wang, H. Ochman, N. A. Moran,
Proc.   Natl.   Acad.   Sci.   U.S.A.   99,  12397  (2002).
7.   B.  L.   Weiss,   Y.   Wu,   J.   J.   Schwank,   N.  S.   Tolwinski,
S.  Aksoy,  Proc.  Natl.  Acad.  Sci.  U.S.A.  105,  15088  (2008).
8.   J.   L.   Round,   S.  K.   Mazmanian,   Nat.   Rev.   Immunol.   9,
313  (2009).
9.   J.   V.   Troll   et  al.,   Environ.   Microbiol.   12,   2190  (2009).
10.   C.   Anselme,   A.   Vallier,   S.  Balmand,   M.   O.   Fauvarque,
A.   Heddi,   Appl.   Environ.   Microbiol.   72,   6766  (2006).
11.   A.   Heddi,   H.   Charles,   C.   Khatchadourian,   G.   Bonnot,
P.   Nardon,   J.   Mol.   Evol.  47,   52  (1998).
12.   H.   Charles,   A.   Heddi,   Y.   Rahb,   C.  R.   Acad.   Sci.   324,
489  (2001).
13.   C.   Conord  et  al.,   Mol.   Biol.   Evol.   25,   859  (2008).
14.   Supporting  material   is  available  on  Science  Online.
15.   H.   Charles,   G.  Condemine,   C.   Nardon,   P.   Nardon,
Insect  Biochem.   Mol.   Biol.   27,   345  (1997).
16.   C.   Anselme  et  al.,   BMC  Biol.   6,   43  (2008).
17.   P.   Bulet  et  al.,   J.   Biol.   Chem.  266,   24520  (1991).
18.   A.   Sagisaka,   A.   Miyanoshita,   J.   Ishibashi,   M.   Yamakawa,
Insect  Mol.   Biol.   10,   293  (2001).
19.   P.   Mergaert  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.   103,
5230  (2006).
20.   W.   Van  de  Velde  et  al.,   Science  327,  1122  (2010).
21.   D.   Fourel,   C.   Hikita,   J.   M.   Bolla,   S.  Mizushima,
J.   M.   Pags,   J.   Bacteriol.   172,  3675  (1990).
22.   E.   Chapman  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.  103,
15800  (2006).
23.   H.   Charles,   A.   Heddi,   J.   Guillaud,  C.   Nardon,   P.   Nardon,
Biochem.   Biophys.   Res.   Commun.   239,  769  (1997).
24.   N. A. Moran, Proc. Natl. Acad. Sci. U.S.A. 93, 2873 (1996).
Acknowledgments:   This  work  was  supported  by  INRA,  INSA
de  Lyon,  the  French  ANR-06-BLAN-0316  (EndoSymArt)
and  ANR-2010-BLAN-170101  (ImmunSymbArt),   a
grant  from  Rgion  Rhne-Alpes  (cluster  infectiologie),
and  the  COST  action  FA0701  (Arthropod  Symbioses).
The  data  reported  in  this  paper  are  posted  in  the
supporting  online  material   (14).   colA  (EY122872)  and
colB  (EY122826)  sequences  are  published  in  GenBank.
SPE  omp  sequences  (GenBank  JN575265,   JN575266,
JN575267)  were  provided  by  C.  Dale  and  R.   B.   Weiss
(University  of  Utah)  from  an  ongoing  SPE  genome
sequencing  and  annotation  project  supported  by  NSF
grant  EF-0523818  and  the  Ministerio  de  Educacin  y
Ciencia  project  BFU2006-06003/BMC  to  A.   Moya  and
A.   Latorre  (University  of  Valencia).  We  thank  R.   Gil   and
K.   Oakeson  for  omp  sequence  analysis;   V.   E.  Shevchik,
G.   Condemine,   and  M.   Lemaire  for  supplying  E.   coli
and  S.   cerevisiae  strains;   W.   J.   Miller  and  B.   Loppin  for
critical   reading  of  the  manuscript;   and  V.   James  for
correction  of  English.   Electron  microscopy  was  carried
out  in  Centre  Technologique  des  Microstructures  (UCBL).
This  paper  is  an  homage  to  the  work  of  Paul   Nardon.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/362/DC1
Materials  and  Methods
Figs.   S1  to  S9
Tables  S1  to  S6
References  (25,  26)
13  June  2011;   accepted  7  September  2011
10.1126/science.1209728
Fig. 3. Effects of  colA inhibition with  RNAi on SPE size  and location. (A) Typical forward  scatterarea/
side scatterarea plots showing size ( x axis) and granularity (y axis) of SPE isolated from larvae injected
with  dsRNA-gfp  (left)   and  with  dsRNA-colA  (right).   Three  SPE  populations   were  defined  arbitrarily.
Small-sized cells (P1) and intermediate-sized cells (P2) significantly increased with dsRNA-colA treatment,
whereas  the  population  of  large-sized  cells (P3)  decreased  (c
2
-test,  P  <  0.0001; see percentage values).
The mean size of P2 and P3 significantly decreased (Mann-Whitney test, P < 0.0001), whereas the mean
size of P1 was equal in dsRNA-gfp and dsRNA-colAinjected larvae (Mann-Whitney test,  P = 0.37). (B)
FISH visualization of SPE 9 days (upper panels) and 14 days (lower panels) after larvae were injected with
dsRNA-gfp  (left)   and  dsRNA-colA  (right).   colA  inhibition  resulted  in  SPE  escaping  the  bacteriome  (see
arrows). See table  S4  for  experimental details.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   365
REPORTS
Stochastic  Pulse  Regulation  in
Bacterial  Stress  Response
James  C.   W.  Locke,*  Jonathan  W.  Young,*  Michelle  Fontes,
Mara  Jess  Hernndez  Jimnez,  Michael  B.  Elowitz
Gene regulatory circuits can use dynamic, and even stochastic, strategies to respond to environmental
conditions. We examined activation of the general stress response mediated by the alternative sigma
factor,  s
B
, in individual Bacillus subtilis cells. We observed that energy stress activates  s
B
in discrete
stochastic pulses, with increasing levels of stress leading to higher pulse frequencies. By perturbing
and rewiring the endogenous system, we found that this behavior results from three key features of the
s
B
circuit: an ultrasensitive phosphorylation switch; stochasticity (noise), which activates that switch;
and a mixed (positive and negative) transcriptional feedback, which can both amplify a pulse and switch
it off. Together, these results show how prokaryotes encode signals using stochastic pulse frequency
modulation through a compact regulatory architecture.
G
ene circuits exhibit fluctuations (noise)
in the concentrations of key components
such   as   transcriptional   regulatory   pro-
teins  (1,   2).   Increasingly,   noise  appears  to  play
functional  roles  in  some  systems  (35).  For  ex-
ample,   noise   could  enable   a   subpopulation  of
cells to enter a transient antibiotic-resistant state,
enhancing their survival (6). However, it remains
unclear how genetic circuits use noise to control
cellular  behaviors.  To  address  this  issue,  we  an-
alyzed s
B
, the transcriptional regulator of general
stress response in  Bacillus  subtilis, at the single-
cell level (79). Here, we show how  s
B
controls
its target genes through sustained pulsing, rather
than  continuous   activation;   how  noise  enables
this behavior; and how stress levels modulate the
frequency of these pulses (Fig. 1A).
In prokaryotes, alternative sigma factors form
a  part  of  the  RNA  polymerase  holoenzyme,  di-
recting  it   to  regulons  that   control   distinct   regu-
latory programs (10). s
B
is found in Gram-positive
bacteria   and   impacts   pathogenicity   in   Listeria
monocytogenes and Staphyloccous aureus (11, 12).
In  B.   subtilis,   s
B
activates  more  than  150  target
genes in response to diverse stresses (7, 13).  s
B
is  kept  inactive  by  its  anti-sigma  factor  RsbW
and  is  activated  by  the  anti-anti-sigma  factor
RsbV,   which  can  be  reversibly  phosphorylated
(see   Fig.   1B  for   regulatory   interactions).   To
analyze   s
B
activation  dynamics,   we  constructed
reporter strains incorporating a yellow fluores-
cent reporter (yfp) for  s
B
activity (Fig. 1B) and
used quantitative time-lapse microscopy to follow
s
B
activation in individual cells (14). To quantify
s
B
activity  in  movies,   we  computed  the  P
sigB
promoter  activity,  defined  as  the  rate  of  produc-
tion of yellowfluorescent protein (YFP) [fig. S1A
and supporting online material (SOM)].
We first measured the response of  s
B
to my-
cophenolic  acid  (MPA),   an  energy  stress  trans-
duced  by  RsbQP  (fig.   S2)  (15).   Constant  MPA
led  to  pulses  of  s
B
activation  in  individual  cells
(Fig.  1,  C  and  D,  and  movie  S1).  These  pulses
were unsynchronized across the population, spo-
radic in time, and sustained, continuing through-
out   the  movie  (about  six  generations)  (fig.   S3).
Similar behavior was observed with other energy
stresses and during growth in liquid culture (figs.
S1  and  S4).   Pulses  reflected  changes  in  s
B
ac-
tivity and not intrinsic variability of the P
sigB
-YFP
promoter   (fig.   S5).   Increasing  MPA  concentra-
tion caused a strong increase in pulse frequency,
with  weaker  increases  in  mean  pulse  amplitude
and duration (Fig. 1E and fig. S6), showing that
s
B
is regulated predominantly by frequency mod-
ulation (FM) in response to energy stress (Fig. 1A).
Pulse  amplitudes  exhibited  broad  and  monoton-
ically increasing variability with increasing MPA,
Howard Hughes Medical Institute, Division of Biology and Bio-
engineering, Broad Center, California Institute of Technology,
1200 East California Boulevard, Pasadena, CA 91125, USA.
*These  authors  contributed  equally  to  this  work.
To  whom  correspondence   should  be   addressed.   E-mail:
melowitz@caltech.edu
Fig.   1.   Energy stress modulates the frequency of stochastic pulses of  s
B
ac-
tivation.  (A)  Schematic  of  FM  pulse  regulation.  The  input  signal (black  line)
controls  the  frequency  of  stochastic  pulses  (blue  line,  schematic).  (B)  Sche-
matic diagram of  s
B
regulatory interactions and states (7). When RsbV (V) is
phosphorylated (OFF state),  s
B
is sequestered by RsbW (W) and inactive (28).
Under energy stresses such as MPA, RsbV is dephosphorylated by the RsbQP
phosphatase complex (QP) (29). Other stress inputs are mediated by the RsbTU
phosphatase complex (not shown; see SOM text for discussion). Dephosphoryl-
ated RsbV can bind to RsbW, releasing  s
B
to activate target genes, including
its own operon (30), and the yfp reporter (yellow). (C) Promoter activity of the
P
sigB
 -YFP reporter pulses in individual lineages (colored solid lines), and its
mean and standard deviation across all lineages in four data sets (dashed line
and shaded area, respectively). (D) Filmstrip of s
B
activation at 60 mg/mL MPA.
Heterogeneous expression levels of P
sigB
 -YFP reflect pulsing activity. (E) MPA
concentration strongly modulates the mean frequency, while more weakly mod-
ulating the mean amplitude and duration, of pulses. Error bars, mean T SEM. (F)
Pulse amplitude histograms for varying levels of MPA. In (E) and (F), each data
point represents data from four microcolonies, acquired on two different days.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 366
REPORTS
with  coefficients  of  variation  ranging  from  0.16
to 0.70 (Fig. 1F). Together, these results provoke
the  question  of  how  FM  pulse  regulation  is  im-
plemented by the  s
B
regulation circuit.
In  principle,   pulses   could  be   generated  in
two qualitatively distinct ways: They could arise
through amplification of an inherently stochastic
underlying  process  (16,   17).   Alternatively,   they
could  result  from  a  limit  cycle  oscillator  whose
dynamics become erratic due to noise (18). Sys-
tematically reducing cellular noise would distin-
guish between these possibilities, eliminating pulses
in the first case but making them more regular in
the second case.
To  modulate  the  amplitude  of  noise  in  cells,
we created strains that could be induced to grow
into long multinucleoid filaments by  controlling
expression of FtsW, a cell division protein neces-
sary for septation. These cells exhibit similar mean
expression levels of cellular components (fig. S7)
but  reduced  fluctuations  (19),   allowing  us  to  in-
vestigate  how  reduced  noise  affects  pulse  fre-
quency.   In  time-lapse  movies,   we  observed  a
systematic decline in pulse frequency in noise-
reduced (long) cells across a range of energy stress
levels (Fig. 2A and fig. S8), which was also con-
sistent with reduced cell-cell variability in  s
B
ac-
tivity in liquid conditions (Fig. 2B). This reduction
in pulse frequency did not reflect reduced sensi-
tivity to MPA, which had a similar effect on growth
rate in long and short cells (fig. S8). Together, these
results rule out limit cycle models and suggest a
noise-dependent mechanism for pulse generation.
How, then, does the  s
B
circuit amplify noise
to  initiate  discrete  pulses  of  s
B
activity?  To  ad-
dress this question, we analyzed the response of
s
B
to  increased  expression  of  each  circuit  com-
ponent. Up-regulation of kinase (RsbW) and phos-
phatase  (RsbQP)  expression  had  much  stronger
(opposite)  effects  on  s
B
activity  compared  with
up-regulation of RsbV (fig. S9). This result is in-
teresting  because  opposing  kinase  and  phos-
phatase  activities  can  generate  sharp,  switchlike
responses   in  the  phosphorylation  of   their   sub-
strate. An extreme example is zero-order ultrasen-
sitivity, where the phosphatase and kinase operate
at  saturation  (2022).  We  found  that  s
B
activity
exhibited  an  ultrasensitive  response  to  inducible
phosphatase concentration (Fig. 2Cand fig. S10),
with  an  effective  Hill   coefficient   of   2.12  [95%
confidence interval (CI),  n
H
 = 2.09 to 2.15]. Sim-
ilar  results  were  also  observed  with  the  RsbTU
phosphatase  (fig.   S11).   Moreover,   this  ultrasen-
sitivity was not due to the transcriptional feedback
loop.   It   could  be   observed  in  an   open-loop
strain, in which operon expression was inducible
and  independent  of  s
B
(fig.  S12).  In  this  strain,
increasing  operon  expression  led  to  increasing
ultrasensitivity  to  phosphatase level. These  ef-
fects could be explained by a minimal mathemat-
ical  model  of  the  phosphoswitch  that  does  not
include the detailed dynamics of the network (see
SOM). Finally, consistent with this model, ectopic
expression of the kinase RsbWshifted the switch-
ing point to higher phosphatase expression levels
(fig. S13). This ultrasensitive phosphoswitch could
Fig. 2. Pulsing is noise-dependent and involves an ultrasensitive phospho-
switch. (A) Pulse frequency in long cells (green) is strongly reduced com-
pared with short cells (gray; data replotted fromFig. 1E). Error bars, mean T SEM.
(B)  Variability  in  P
sigB
  -YFP  expression  decreases  with  increasing  cell  length
(see fig. S8). Equal numbers of cells (represented by dots) are plotted in each
log-spaced  bin  (delimited  by  gray  vertical   lines).   (Inset)   Overlay  of   phase
contrast  and  P
sigB
  -YFP  expression  (green)  at  different  cell  lengths.  Note
greater   s
B
variability  in  short  cells.   (C)   s
B
expression  is  ultrasensitive  to
RsbQP phosphatase levels. Each dot represents the mean RsbQP-YFP level and
P
sigB
 -CFP level of one cell, using the strain shown schematically (table S1). The
red line is a Hill function with Hill coefficient n
H
 = 2.12 (95% CI, n
H
 = 2.09 to
2.15).
Fig.   3.   A  mixed  transcriptional   feedback   loop  amplifies   and  terminates
pulses. (A) Schematic diagram  of supra- and subthreshold  protocols. Before
time-lapse  acquisition  (gray  region),   phosphatase  is  induced  to  a  constant
level   by  addition  of   xylose.   After  the  start   of   acquisition,   isopropyl-b-D-
thiogalactopyranoside (IPTG) is added to induce rsbVWB to levels greater than
(solid  red  line)  or  less  than  (dashed  red  line)  the  level  of  phosphatase.  This
results in pulsed (solid green line) or sustained (dashed green line) s
B
activity
dynamics.   (B)   s
B
promoter  activity  exhibits  a  transition  between  sub-  and
suprathreshold behaviors. Each trace shows the mean P
sigB
 promoter activity
averaged  over four colonies. The promoter  activity of  the IPTG-inducible  s
B
operon  ( x  axis)  was  estimated  using  a  separate  strain  containing  a  similar
IPTG-inducible  yfp  reporter.   Two  repeat   movies   showed  similar   behaviors.
(Inset) Schematic diagram of strain used for this experiment (table S1). (C) A
minimal mathematical model of the open-loop s
B
network reproduces the main
features of the experimental data. (Inset) In this model, the unphosphorylated
activator, A, directly activates target genes (see SOM).
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   367
REPORTS
activate s
B
in response to fluctuations in the phos-
phatase/kinase ratio and thereby initiate pulses.
How are s
B
pulses further amplified and sub-
sequently  terminated?  s
B
activates  its  own  ope-
ron  (rsbV-rsbW-sigB).  This feedback  loop  could
increase  s
B
activity, due to the activating effects
of  RsbV and  s
B
,  or  it  could  repress  s
B
activity,
due  to  increased  production  of   RsbW.   We  hy-
pothesized that the phosphoswitch sets a thresh-
old  between  activating  (phosphatase  dominant)
and  repressing  (kinase  dominant)   feedback  re-
gimes.  As  long  as  phosphatase  activity  exceeds
kinase activity, activation of the operon increases
free s
B
(positive feedback). However, this also in-
creases production of RsbW kinase. When kinase
activity  approaches  that   of  the  phosphatase,   in-
creased operon expression will cause RsbWlevels
to  cross  the  threshold,   shutting  off   activation
(negative  feedback).  Thus,  autoregulation  could
result in a  mixed (positive and negative) feed-
back  loop,   providing  a  compact   mechanism  to
first amplify and then terminate a pulse (23).
To  test   this   hypothesis,   we   constructed  an
open-loop strain and quantified the change in  s
B
activity  in  response  to  a  step  increase  in  operon
expression.  In  these  experiments,  we  first  estab-
lished  a  basal   level   of   phosphatase  activity  in
cells and subsequently induced a step, of varying
size, in  s
B
operon expression (Fig. 3A). We ob-
served a striking transition between two qualita-
tively different responses: At lower operon induction
levels, the system produced a sustained response,
whereas at higher induction levels, it exhibited a
pulse (Fig. 3B). These results are consistent with
the  mixed  feedback  model:  Initially,  increased
operon  induction  produces   more   s
B
,   which  is
active due to the high levels of phosphatase, en-
gaging  the  positive  feedback  loop.   For   lower
(subthreshold) operon induction levels, RsbWlev-
els  never  exceed  phosphatase  levels,  so  the  sys-
temremains on indefinitely (Fig. 3A, dashed lines).
In contrast, at higher induction levels (superthresh-
old), RsbWactivity eventually crosses the thresh-
old set by the phosphatase and thereby shuts the
system  off,   resulting  in  a  pulse  (Fig.   3A,   solid
lines).   Indeed,   RsbW  dominated  other  operon
components at steady state, suppressing  s
B
ac-
tivity  in  a  dose-dependent   manner  (fig.   S9).   In
this mechanism, pulse amplitude should be rough-
ly proportional to the difference between the phos-
phatase  level   and  the  kinase  level   immediately
after  the  initiating  fluctuation,   as  confirmed  ex-
perimentally (fig. S14). A minimal mathematical
model of the circuit exhibited qualitatively simi-
lar behavior (Fig. 3C). This mechanism for pulse
initiation, amplification, and termination is sum-
marized in Fig. 4, A and B.
These  results  provoke  a  final  question:  How
can the cell modulate the frequency of pulses in
this system? Systematic changes in the activity of
either kinase or phosphatase could modulate the
likelihood of threshold-crossing events and there-
by control pulse frequency. We first examined the
distribution of RsbQP expression levels, using a
P
rsbQP
-rsbQP-YFP protein fusion that complements
an RsbQP null mutant (fig. S15). In response to
40  mg/ml  MPA,  we  observed  a  ~3-fold  increase
in  mean  RsbQP-YFP  levels,   and  a  ~6-fold  in-
crease in mean  s
B
activity (fig. S16, A  and B).
At the single-cell level, RsbQP-YFP expression
mapped  to  s
B
activity  (fig.   S16C),   closely  fol-
lowing  the  (independently determined)  ultrasen-
sitive  response  function  (Fig.  2C).  These  results
suggest  that  stress  increases  s
B
pulse  frequency
by  increasing  the  distribution  of  RsbQP  expres-
sion levels and thereby increasing the frequency
with which RsbQP fluctuations cross the thresh-
old set by RsbW (Fig. 4C). These results do not
rule out the complementary possibility, suggested
previously  (24),   that   some  energy  stresses  may
activate  s
B
by reducing kinase activity.
To  show  that  this  mechanism  is  indeed  suf-
ficient   to  enable  frequency  modulation,   we  re-
wired  the  endogenous  circuit,   replacing  RsbQP
with  an  inducible,   constitutively  active  RsbTU
phosphatase complex that was unaffected by en-
ergy  stress  (Fig.  4D,  inset).  The  rewired  system
exhibited stochastic pulsing in response to RsbTU
expression  (figs.   S17  and  S18  and  movie  S2).
Furthermore, we observed an increased frequen-
cy  of   pulsing  in  response  to  increased  RsbTU
phosphatase  expression  (Fig.   4D),   with  weaker
effects on pulse amplitude and duration (fig. S20).
These  results,   qualitatively  similar   to  those  ob-
served in wild-type cells under energy stress, also
match  an  extended  mathematical  model  that  in-
cludes   the   wild-type   transcriptional   feedback
(gray dashed lines in Fig. 4D, figs. S19 and S20)
(see SOM). Thus, modulation of phosphatase ex-
pression is sufficient to recapitulate FM pulsing,
and  no  special  property  of  the  RsbQP  phospha-
tase is required.
Fig.  4.  Mechanism of FM pulse con-
trol. (A) Schematic time course of phos-
phatase  RsbQP  (denoted  P,   purple),
free  s
B
(s
B
,   green),   and  kinase  (W,
red) during a pulse cycle. Circled num-
bers indicate specific steps in (B). (B)
Schematic  diagram  of  pulse  control.
The relative concentration of each com-
ponent is indicated by size. (1) Initial
state: System components are at low
levels, kinase activities exceed phos-
phatase activities, and therefore RsbV
is mostly phosphorylated. A threshold-
crossing upward fluctuation in RsbQP
level dephosphorylates V
P
, leading to
(2)  Pulse  Initiation.  Activation  of   s
B
(indicated  by  glowing  halo)  leads  to
up-regulation of operon components
(operon feedback). (3) Pulse peak: s
B
activity peaks just before RsbWkinase
activity exceeds phosphatase activity.
(4)   Termination:   Rephosphorylation
of RsbV shuts the system off. (5) Di-
lution: Component levels reset to the
original state. (C) Mechanismof frequen-
cy modulation. Fluctuations in phos-
phatase level (purple arrow from state 1 to 2) can cross the kinase threshold
(red  line)  to  initiate  a pulse, with  amplitude determined  by  the size  of  fluc-
tuation  (dashed  line). Increased  stress  shifts  the distribution  of  phosphatase
levels   from  lower   to  higher   values   (dark  and  light   gray,   respectively),   in-
creasing  the  frequency  of  threshold-crossing  events  and  thereby  increasing
pulse frequency (inset). (D) Tuning of phosphatase expression by IPTG (strain
indicated  schematically  in  inset)  can  regulate  pulse  frequency.  Gray  dashed
lines show a similar behavior for the mathematical model (fit to data). Each
data point represents statistics fromtwo colonies. Two repeat data sets showed
similar trends.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 368
REPORTS
FM pulsing can be implemented by a simple
circuit of three genes (rsbW, rsbV, and sigB), with
input  from  a  phosphatase  complex.  This  system
provides a fundamental signal-processing capabil-
ity  to  bacterial   cells,   enabling  them  to  convert
steady  DC inputs into pulsatile, predominantly
AC outputs. Noise plays a key functional role
in this signal  processing system (3). The  s
B
cir-
cuit   conserves  its  core  architecture  in  diverse
bacteria  (7),   and  other  alternative  sigma  factors
similarly feature both posttranslational regulation
by  anti-sigma  factors   and  autoregulatory  feed-
back.   Thus,   related  stochastic  pulse  modulation
schemes  are  likely  employed  more  generally  in
bacteria (10). The relatively slowtime scale of s
B
pulses  (Fig.   1E)  could  confer  advantages  in  re-
sponding to unpredictable environments and main-
taining a broad, but dynamic, distribution of states
in  the  population  through  bet-hedging  (25,   26).
Given  the   negative   effect   of   s
B
activation  on
growth rate in some conditions, even under energy
stress (27), these results suggest that cells balance
the  benefits  and  costs  of  s
B
activation  dynami-
cally.  It  will  be  interesting  to  see  whether  other
dynamic  encoding  schemes  are  similarly  imple-
mented by relatively simple circuit modules.
References  and  Notes
1.   A.   Raj,   A.   van  Oudenaarden,   Cell   135,   216  (2008).
2.   N.   Rosenfeld,   J.   W.   Young,   U.  Alon,   P.   S.  Swain,
M.   B.   Elowitz,   Science  307,   1962  (2005).
3.   A.   Eldar,   M.   B.  Elowitz,  Nature  467,  167  (2010).
4.   R.   Losick,   C.   Desplan,   Science  320,  65  (2008).
5.   L.   Cai,   C.   K.   Dalal,   M.   B.  Elowitz,   Nature  455,  485
(2008).
6.   E.   Rotem  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.   107,
12541  (2010).
7.   M. Hecker, J. Pan-Farr, U. Vlker, Annu. Rev. Microbiol.
61,  215  (2007).
8.   W.   G.   Haldenwang,   R.   Losick,   Nature  282,   256
(1979).
9.   O.   A.   Igoshin,   M.   S.   Brody,   C.   W.   Price,   M.   A.   Savageau,
J.   Mol.   Biol.   369,  1333  (2007).
10.   T.   M.   Gruber,   C.  A.   Gross,   Annu.   Rev.   Microbiol.   57,
441  (2003).
11.   M. J. Kazmierczak, S. C. Mithoe, K. J. Boor, M. Wiedmann,
J.   Bacteriol.   185,  5722  (2003).
12.   U.   Lorenz  et   al.,   Microbes  Infect.   10,   217  (2008).
13.   M.   Hecker,   U.   Vlker,   Mol.   Microbiol.   29,   1129
(1998).
14.   J.   C.   Locke,   M.   B.  Elowitz,   Nat.   Rev.   Microbiol.   7,  383
(2009).
15.   S.   Zhang,   W.   G.   Haldenwang,   J.   Bacteriol.   187,  7554
(2005).
16.   A.  L.  Hodgkin,  A.  F.  Huxley,  J.  Physiol.  117,  500  (1952).
17.   G.   M.   Sel,   J.   Garcia-Ojalvo,   L.   M.  Liberman,
M.   B.   Elowitz,   Nature  440,   545  (2006).
18.   M.   B.   Elowitz,   S.   Leibler,   Nature  403,  335  (2000).
19.   G.   M.   Sel,   R.   P.   Kulkarni,   J.   Dworkin,   J.   Garcia-Ojalvo,
M.   B.   Elowitz,   Science  315,   1716  (2007).
20.   A.   Goldbeter,   D.   E.  Koshland  Jr.,   Proc.  Natl.   Acad.
Sci.   U.S.A.   78,  6840  (1981).
21.   G. J. Melen, S. Levy, N. Barkai, B. Z. Shilo, Mol. Syst. Biol.
1,  2005.0028  (2005).
22.   Z.   Cheng,   F.   Liu,   X.   P.   Zhang,   W.   Wang,  Biophys.   J.
97,   2867  (2009).
23.   J. C. Ray, O. A. Igoshin, PLOS Comput. Biol. 6, e1000676
(2010).
24.   S.   Alper,   L.   Duncan,   R.   Losick,   Cell   77,   195
(1994).
25.   M.   Acar,   A.   Becskei,   A.   van  Oudenaarden,   Nature  435,
228  (2005).
26.   E.   Kussell,   S.   Leibler,   Science  309,   2075  (2005).
27.   T.   Schweder,   A.   Kolyschkow,   U.  Vlker,  M.   Hecker,
Arch.   Microbiol.   171,  439  (1999).
28.   A.   Dufour,   W.   G.   Haldenwang,   J.  Bacteriol.  176,   1813
(1994).
29.   M.   S.  Brody,   K.   Vijay,   C.   W.   Price,   J.   Bacteriol.   183,
6422  (2001).
30.   A.   A.   Wise,   C.   W.   Price,   J.   Bacteriol.   177,   123
(1995).
Acknowledgments:   We  thank  C.   Price  and  D.   Rudner  for
providing  strains.  We  thank  A.  Eldar,  R.  Kishony,  C.  Price,
N.  Wingreen,  J.  Levine,  and  other  members  of  M.B.Es
laboratory  for  helpful  discussions.  Work  in  M.B.Es
laboratory  was  supported  by  NIH  grants  R01GM079771
and  P50  GM068763,  U.S.  National  Science  Foundation
CAREER  Award  0644463,  and  the  Packard  Foundation.
J.C.W.L  was  supported  by  the  International  Human
Frontier  Science  Program  Organization  and  the  European
Molecular  Biology  Organization.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1208144/DC1
Materials  and  Methods
SOM  Text
Figs.   S1  to  S20
Table  S1
References
Movies  S1  and  S2
10  May  2011;   accepted  1  September  2011
Published  online  6  October  2011;
10.1126/science.1208144
Transgenerational  Epigenetic
Instability  Is  a  Source  of
Novel  Methylation  Variants
Robert  J.  Schmitz,
1,2
Matthew  D.  Schultz,
1,2,3
Mathew  G.  Lewsey,
1,2
Ronan  C.   OMalley,
2
Mark  A.  Urich,
1,2
Ondrej  Libiger,
4
Nicholas  J.  Schork,
4
Joseph  R.  Ecker
1,2,5
*
Epigenetic  information,  which  may  affect  an  organisms  phenotype,  can  be  stored  and  stably
inherited  in  the  form  of  cytosine  DNA  methylation.  Changes  in  DNA  methylation  can  produce
meiotically stable epialleles that affect transcription and morphology, but the rates of spontaneous
gain  or  loss  of  DNA  methylation  are  unknown.  We  examined  spontaneously  occurring  variation
in  DNA  methylation  in  Arabidopsis  thaliana  plants  propagated  by  single-seed  descent  for  30
generations.  We  identified  114,287  CG  single  methylation  polymorphisms  and  2485  CG  differentially
methylated  regions  (DMRs), both  of which  show  patterns of  divergence  compared  with the  ancestral
state.  Thus,  transgenerational  epigenetic  variation  in  DNA  methylation  may  generate  new  allelic
states  that  alter  transcription,  providing  a  mechanism  for  phenotypic  diversity  in  the  absence  of
genetic  mutation.
C
ytosine methylation is a DNA base mod-
ification  with  roles  in  development   and
disease in animals as well as in silencing
transposons   and  repetitive   sequences   in  plants
and fungi (1). In plants, CG methylation is com-
monly  found  within  gene  bodies  (25),  whereas
non-CG  methylation,  CHG  and  CHH  (where  H
is  A,  C,  or  T),  is  enriched  in  transposons  and  re-
petitive  sequences  (1).  The  RNA-directed  DNA
methylation  (RdDM)   pathway  targets  both  CG
and  non-CG  sites  for   methylation  and  is  com-
monly  associated  with  transcriptional   silencing
(6).   This   pathway  can  also  target   and  silence
protein-coding genes, giving rise to epigenetic al-
leles  or  so-called  epialleles  that  can  be  heritable
through mitosis and/or meiosis (7,  8) and can be
dependent on the methylation of a single CG di-
nucleotide  (9).
Two  meiotically  heritable  epialleles  result-
ing  in  morphological  variation  are  the  peloric
(Linaria  vulgaris)   and  colorless   non-ripening
(Solanum  lycopersicum) loci (10,  11). Both show
spontaneous  epigenetic  silencing  events  within
their respective populations (10,  12). However, the
frequency at which such spontaneous meiotically
heritable  epialleles  naturally  arise  in  populations
is unknown. Although epiallelic variation has been
identified between genetically diverse populations
within  Arabidopsis   thaliana  (13),   it   is   unclear
whether   these   identified   epialleles   are   due   to
underlying  genetic  variation.  Epialleles  have  al-
so  been  artificially  generated  after  mutagenesis
or   because  of   mutations   in  the  cellular   com-
ponents  required  for  the  maintenance  of  DNA
methylation  (1416).
An  A.  thaliana (Columbia-0) population, the
MA lines, derived by single-seed descent for 30
generations (17) was used to examine the extent
of naturally occurring variation in DNA methyla-
tion and the frequency at which spontaneous epi-
alleles emerge over time. We used the MethylC-Seq
method  (3)  to  determine  the  whole-genome base
resolution  DNA  methylomes  for   three  ancestral
1
Plant   Biology   Laboratory,   The   Salk   Institute  for   Biological
Studies,   La  Jolla,   CA  92037,   USA.
  2
Genomic  Analysis  Labo-
ratory,   The  Salk  Institute  for  Biological   Studies,   La  Jolla,   CA
92037, USA.
 3
Bioinformatics Program, University of California
at San  Diego, La Jolla, CA 92093, USA.
  4
The Scripps Transla-
tional Science Institute and the Department of Molecular and
Experimental   Medicine,   The   Scripps   Research   Institute,   La
Jolla, CA 92037, USA.
  5
Howard Hughes Medical Institute, The
Salk Institute for Biological Studies, 10010 North Torrey Pines
Road,  La  Jolla,  CA  92037,  USA.
*To  whom  the  correspondence  should  be  addressed.   E-mail:
ecker@salk.edu
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   369
REPORTS
MA  lines   (numbers   1,   12,   and   19)   and   five
descendant  MA  lines  (numbers  29,  49,  59,  69,
and 119) (fig. S1). We refer to lines 1, 12, and 19
as   ancestors   throughout   this   study,   although
they  are  not   direct   ancestors  because  they  are
three  generations  removed  from  the  original
founder line (fig. S1). These specific descendant
lines were  selected  because  their genomes  have
been  sequenced  and  they  have  a  known  level  of
spontaneous mutation (18). Biological replicates
(sibling  plants)  for  each  leaf  methylome  were
sequenced to an average of ~34-fold coverage,
which  allowed  for   an  average  per   line  exami-
nation  of  39,897,093  (96.35%)  uniquely  mapped
cytosines and 5,307,077 (98.39%) uniquely mapped
CGs  (table  S1).
A  total  of  1,730,761  CGs  were  methylated
(mCGs) in at least one MA line (Fig. 1A), and
about   91%  of  the  covered  mCGs  were  invar-
iably  methylated  across  all  eight  lines  (19).  The
variable  mCGs  revealed  a  set   of  114,287  high-
confidence CG single methylation polymorphisms
(SMPs)  that  showed  a  consensus  of  the  meth-
ylation  status  of   CG  dinucleotides  between  bi-
ological  replicates  (Fig.  1A).  Next,  a  reference
MA founder DNA methylome was created by
pooling  the   completely  conserved  mCG  site
calls  for  all  ancestral  MA  lines  and  used  to  de-
termine   the  frequency  of   discordant   CG-SMP
sites within the descendant population (Fig. 1B).
Within  the  descendant  lines,  ~1.62%  of  the  CG
methylome  shows  susceptibility  to  dynamic  ac-
quisitions  and  losses  of   mCGs  over   time  (table
S2).   On  average,  ~66,000  methylated  CG-SMPs
(mCG-SMPs)   were  identified  for   each  ances-
tral  and descendant line (fig. S2). Although the
total   number   of   mCG-SMPs   was   similar   be-
tween  all   lines,   the  conservation  of   these  poly-
morphisms  among  and  between  ancestral   and
descendant   populations   was   different   (Fig.   1C
and  table  S3).   A  pairwise  comparison  of   both
populations  for  methylation  conservation,   esti-
mated  by  global   similarity  of   mCG-SMP  sites
(19),   revealed  that   all   of   the  ancestral   lines   are
highly similar (table S4). Descendant lines showed
greater  similarity  in  CG-SMPs  methylation  sta-
tus  to  ancestral  lines  than  to  other  descendant
lines  (table  S4).
We calculated an estimate of the epimutation
rate  per   generation  in  this  population  by  using
linear  regression  and  TREE  PUZZLE,  which  re-
vealed  704  and  2876  methylation  changes  each
generation, respectively (19). We estimated a lower
bound  of   the   epimutation  rate   with  the   linear
regression  results,  which  revealed  4.46    10
4
methylation polymorphisms per CG site per gen-
eration  (P  <  0.0000216)  (table  S5).  This  finding
contrasts  with  the  previously  reported  spontane-
ous  genetic  mutation  rate  of  7    10
9
base  sub-
stitutions  per  site  per  generation  for  these  same
MA  lines (18).  The TREE  PUZZLE  analysis re-
vealed higher estimated epimutation rates in earlier
generations (19). One possible source of this var-
iation  could  be  due  to  seed  age,  storage,  and/or
selection for seed survival. Therefore, although
DNA  methylation  is   predominantly  static   over
relatively long periods  of  time, changes  in cyto-
sine  methylation  do  occur   and  at   a  frequency
greater   than   that   of   mutation   observed   at   the
DNA  sequence  level.
By  using  CG-SMPs  derived  from  both  an-
cestral and descendant populations, we carried
out a genome-wide analysis of differentially meth-
ylated regions (DMRs) and identified 2485 CG-
DMRs  that  ranged  in  size  from  11  to  1110  base
pairs  (bp)   (Fig.   2A  and  table  S6).   Hierarchical
clustering  of  CG-DMRs  in  this  population,   cal-
culated   solely   on   the   basis   of   the   methylation
density,  revealed  that  the  ancestral  lines  segregate
as  an  independent   cluster   from  the  descendant
lines  (Fig.  2B  and  fig.  S3).  Multivariate  distance-
based  regression  (MDMR)  (20,   21)  confirmed
this  finding,   indicating  a  statistically  significant
(P  <  0.00005)   association  between  ancestor   or
descendant status and methylation density of the
CG-DMR  profiles.   The  ancestor   or  descendant
status  explained  47%  of  the  variance  in  the  dis-
similarity  in  methylation  density  of   CG-DMRs
between  pairs  of   samples,   indicating  that,   over
time,  there  is  a  divergence  of  DNA  methylation
patterns in both formation and elimination of CG-
DMRs. Furthermore, the genome-wide locations
of these CG-DMRs were not uniformly distributed
(P < 2.20  10
16
), because 60.5% (1504/2485)
were found in genic regions compared with 3.3%
(82/2485)  and  36.2%  (899/2485)  located  in  in-
tergenic  regions  and  transposons,  respectively
(Fig.   2B).
Next,   we  performed  a  genome-wide  survey
for  nonCG-DMRs  and uncovered a total  of  284
among  all  eight  lines  (table  S7).  In  general,  the
nonCG-DMRs   were   largely  localized  to  inter-
genic regions (141/284) of the genome, because
only  57/284  overlapped  with  genes  and  86/284
overlapped with transposons. The size ranges of
the  nonCG-DMRs  were  similar  to  those  of  the
CG-DMRs because the vast majority occurred in
smaller segments of the genome (10 to 682 bp).
Therefore,   variation   in   DNA  methylation   ap-
pears  to  occur  in  all  three  methylation  sequence
contexts.
CG methylation is present within gene bodies
and is enriched toward the 3 end (25), whereas
CG  and  nonCG  methylation  is  associated  with
heterochromatin,   transposons,   and  repetitive  se-
quences (1). In agreement with these findings, we
observed  that   the  3   portion  of  genes  contained
the  greatest   source  of   CG-DMRs   and  that   the
majority  of  nonCG-DMRs  were  enriched  out-
side of the  gene  bodies  (Fig.  2C).  Furthermore,
we  observed  a  ~twofold  depletion  of  CG-DMRs
in exons compared with introns (Fig. 2D). The
genome-wide distributions of CG-SMPs, CG-DMRs,
Fig.  1.  Epigenetic variation of CG-SMPs. (A) An example of a CG-SMP. Gold lines indicate CG methyl-
ation, maroon rectangle indicates the untranslated regions, and green rectangles indicated exons. (B) A
breakdown  of  the  methylation  distribution  of  CG  dinucleotides  among  all  samples.  (C)  A  heatmap  indi-
cating  the  number  of  CG-SMPs  that  differ  between  two  samples  (table  S3).
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 370
REPORTS
and   nonCG-DMRs   were   depleted   in   hetero-
chromatic   regions   in   the   genome   (Fig.   2,   E
and F). These depletions were mostly observed at
the  pericentromeres  and  centromeres  (Fig.   2,   E
and   F,   and   figs.   S4   and   S5).   CG-DMRs   are
enriched  in  transposons  located  in  euchromatin
but   depleted  in  transposons   present   near   the
centromere.  Because  the  centromeric  regions  of
the genome contain the highest density of DNA
methylation (Fig. 2, E and F), these observations
combined with the observations  that  CG-DMRs
are   enriched   in   intron  sequences   may   indicate
that DNA methylation that is associated with nu-
cleosomes (22) (i.e., exons or tightly packaged
chromatin  in  the  pericentromeres  and  centro-
meres)  may  be  maintained  at  a  higher  fidelity
and that DNA methylation not associated with
nucleosomes   may  undergo  greater   epigenetic
drift.
A  genome-wide  screen  for   DMRs   simulta-
neously occurring in all three methylation sequence
contexts   (C-DMRs   are   CG,   CHG,   and  CHH)
was  performed  to  assess  the  extent  of  epiallelic
variation  that   is  characteristic  of   RdDM  across
the MA population. In total, 72 C-DMRs were
identified,   of   which  functional   categorization
revealed  that   two-thirds  overlapped  with  trans-
poson  and  intergenic  sequences  whereas  about
one-third  overlapped  with  gene  bodies  and  pro-
moters  (Fig.   3A  and  table  S8).   To  determine
whether  transposition-induced  methylation  could
potentially  give  rise  to  the  methylated  C-DMRs
(mC-DMRs) (23), genomic DNA encompassing
all  C-DMRs  was  amplified  and  compared  in  all
ancestral   and  descendant   lines.   In  every  case,
the  observed  amplicon  size  was  identical   for
all  MA lines and was equal to the expected size
of   the  locus   (table   S8),   indicating  that   these
C-DMRs  are  unlinked  to  cis-genetic  variation
located  within  500  bp,  a  distance  that  would  be
expected to reveal methylation induced by trans-
poson  insertions  at  these  loci  (23).  Additionally,
none of the genetic variants identified by genome
resequencing  of  this  population  (18)  overlapped
with  any  of  these  C-DMRs.   Lastly,  restriction
enzyme  digestion  and  Southern  blot   analyses
were  performed  to  rule  out  the  possibility  that
copy  number   variants  were  the  cause  of   spon-
taneous epiallele formation, as is the case for the
PAI epialleles (24). In all cases examined, the ob-
served hybridization pattern and gene copy num-
ber   were   identical   for   each  of   the  MA  lines
(fig.   S6).   Therefore,   we  conclude  that   the  72
C-DMRs represent a set of spontaneously occur-
ring epialleles within the MA lines, because they
were  not  associated  with  any  genetic  variation.
By  using  a  set   of   C-DMRs  that   exhibited
an  identical  methylation  status  (fig.  S7),  we  de-
termined   the   frequency   of   discordance   of   the
ancestral state with the descendant lines and found
that  29  of  the  C-DMRs  were  highly  variable  (>1
descendant   line  was  discordant   with  the  ances-
tral state) (Fig. 3B). C-DMRs discordant in only
one  of  the  five  descendant   lines  were  the  most
frequent   class,   but   there   was   an  unexpectedly
high  number  of  C-DMRs  (63%)  that   were  dis-
cordant  in  more  than  one  descendant  (Fig.  3B).
Within  the  set  of  576  C-DMRs  identified  (eight
lines by 72 C-DMRs), 7 were discordant between
the biological  replicates  (table  S8). These  data
suggest  that,  although  many  C-DMRs  represent
the  formation  of  spontaneous  epialleles,  a  small
subset   may  reflect   the  presence  of   hotspots
(metastable  epialleles).
We  sequenced  small   RNA  (smRNA)  pop-
ulations   for   all   eight   lines   and   found   that
smRNAs  [represented  as  RPKCMs  (reads  per
kilobase  of   each  C-DMR  per   million  reads)   in
Fig.  2.  CG-DMRs diverge over time and are enriched in
gene bodies. (A) Example CG-DMR present in an unmeth-
ylated  state  in  both  replicates  of  line  69.  (B)  A  heatmap
representation  of   a  two-dimensional   hierarchical   cluster-
ing  based  on  DMRs.   Columns  represent   samples.   Rows
indicate  DMRs.   The  column  to  the  left   of   the  heatmap
indicates  the  genomic  location  of  the  DMR  (blue,   gene
body; gold, transposon; gray, intergenic; red, transposon
in  gene  body).  (C)  The  average  distribution  of  CG-DMRs
(red) and nonCG-DMRs (blue) across gene bodies (from the start of the 5 UTR to the end of the 3 UTR, including 500 bp up- and downstream). (D) CG gene-
body DMRs are specifically depleted in exons. (E) Genome-wide distributions of mCG (red), CG-SMPs (green), and CG-DMRs (blue) across chromosome I. (F)
Genome-wide  distributions  of  methylated  nonCGs  (mnonCG,  red)  and  nonCG-DMRs  (green)  across  chromosome  I.  The  centromere  is  indicated  by  the  pink
vertical  bar  for  (E)  and  (F).
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   371
REPORTS
tables   S9   to   12]   were   associated   with   an   in-
crease   in  the  average   methylation  density  of
C-DMRs (Fig. 3C). Furthermore, this association
resembled   a   binary   switch,   because   the   most
densely   methylated   C-DMRs   contained   abun-
dant  24-nucleotide  (nt)  smRNAs  (Fig.  3C).
Of   the   eight   previously   documented   plant
epialleles resulting in phenotypic variation, all af-
fected  transcriptional   output   of   the  differentially
methylated  locus   (911,   2328).   mRNA  abun-
dance was measured in all eight lines with quan-
titative   reverse   transcription   polymerase   chain
reaction (qRT-PCR) at eight C-DMRs that over-
lapped  with  protein-coding  regions.   In  four   of
these genes, the gain or loss of DNA methylation
was  correlated  with  a  large  decrease  or  increase
in  mRNA  abundance,   respectively,   and  with  the
presence  of  24-nt  smRNAs  at  each  silenced  epi-
allele  (Fig.   3,   D  to  F,   and  fig.   S8).   These  find-
ings   reveal   that   changes   in  epiallelic  state  can
lead  to  major   effects   on  transcriptional   output
(fig.  S9).
We  also  observed  that  the  methylation  sta-
tus  of  one  C-DMR  resulted  in  alternative  pro-
moter usage of  ACTIN RELATED  PROTEIN 9
(At5g43500) (fig. S10C). The loss of DNA meth-
ylation  within  the  5   untranslated  region  (UTR)
of the At5g43500.1 isoform led to an increase in
mRNA expression, whereas expression of iso-
form  At5g43500.2,   with  a   transcriptional   start
site  located  further  downstream,  was  unaffected
(fig.  S10,  D  and  E).
Although  epialleles  can  have  major  impacts
on  phenotypic  diversity,   until   now  their   identi-
fication  was not  trivial.  Even  more puzzling  is
the  origin  of   pure  alleles,  which  are  defined
by their formation in the absence of any genetic
variation  in  cis  or   trans  (8).   One  route  to  epi-
allele  formation  may  be  the  failure  to  correctly
maintain  the  proper  methylation  status  through-
-1 0 1 2 3 4 5 6 7 8
A   B
Transposons
n = 27
Intergenic
n = 21
Genes
n = 14
Promoters
n = 7
ncRNAs
n = 2
Pseudogene
n = 1
# of descendant lines 
discordant with ancestral state
0
2
4
6
8
10
12
14
16
18
1 2 3 4 5
Methylated Unmethylated
D   E
1 rep1
1 rep2
19 rep1
19 rep2
12 rep1
12 rep2
29 rep1
29 rep2
49 rep1
49 rep2
59 rep1
59 rep2
69 rep1
69 rep2
119 rep1
119 rep2
A
n
c
e
s
t
o
r
s
D
e
s
c
e
n
d
a
n
t
s
Log2 fold change in mRNA levels 
of At5g24240 (relative to line 1)
At5g24240
At5g24250
1
19
12
29
49
59
69
119
N
u
m
b
e
r
 
o
f
 
C
-
D
M
R
s
C
F
24nt
23nt
22nt
21nt
1
19
12
29
49
59
69
119
smRNA levels at At5g24240 C-DMR (RPKCMs)
0 2 4 6 8 10 12 14 16
mC-DMR density quantiles (%)
A
v
e
r
a
g
e
 
s
m
R
N
A
 
R
P
K
C
M
s
0
2
4
6
8
10
12
14
10 20 30 40 50 60 70 80 90 100
21nt
22nt
23nt
24nt
Fig.  3.  Epiallelic variation at protein-coding loci is associated  with  transcrip-
tional variation. (A) Classification of C-DMRs and their genomic locations. (B)
The  number  of  descendant  lines  discordant  with  the  ancestral   C-DMR  state
and the C-DMR methylation status. The black portions of the bar indicate the
descendant   C-DMRs   that   became   methylated,   whereas   the   white   portions
indicate regions that became unmethylated, compared with the ancestral pop-
ulation. (C) The 24-nt smRNA levels are associated with increasing methyla-
tion density. The 24-nt smRNA RPKCMs for all 576 C-DMRs (8 MA lines by
72 C-DMRs) were ranked and binned into 10% quantiles, and then the aver-
age  mC  densities  were  plotted.  (D)  A  representative  C-DMR  at  At5g24240  in
which both biological replicates of descendant line 59 were unmethylated. (E)
qRT-PCR analysis of At5g24240 reveals >50-fold increase in mRNA abundance
in  unmethylated  line  59.  Error  bars  indicate  SEM.  (F)  The  24-nt  smRNAs  are
enriched  specifically  in  the  MA  lines  that  are  transcriptionally  silenced  in  (E)
for  the  At5g24240  locus  with  the  exception  of  line  59,  which  is  abundantly
expressed  in (E).
0
10
20
30
40
50
60
met1 ddc
Partially
Methylated
# of mC-DMRs 
that become 
unmethylated in 
# of C-DMRs 
that become 
re-methylated in
rdd
Not 
methylated
in
Col-0
N
u
m
b
e
r
 
o
f
 
C
-
D
M
R
s
Fig.  4.  Methylation status of all 72 epialleles in methylation and demethylation mutant backgrounds.
Most  of   the  epialleles  become  unmethylated  in  met1-3,   whereas  a  smaller  number  become  remeth-
ylated  in  the  DNA  demethylase  triple  mutant  rdd.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 372
REPORTS
out  epigenetic  reprogramming  that   occurs  post-
fertilization  (29,   30).  It  is  noteworthy  that  63  of
the 72 C-DMRs overlap with regions previously
shown  to  have  altered  methylation  patterns   in
methylation enzyme mutants (Fig. 4) (3). Of the
14  C-DMRs  that  overlap  with  genes,  5  become
reexpressed  in  met1-3  and  1  transcript  becomes
silenced  in  rdd  (3).  These  results  suggest  that  a
failure  to  faithfully  maintain  genome-wide  meth-
ylation  patterns  by  MET1  and/or   RDD  is  likely
one  source  of  spontaneous  epiallele  formation.
Regardless of their origin, the majority of epi-
alleles  identified  in  this  study  are  meiotically  sta-
ble  and  heritable  across  many  generations  in  this
population. Understanding the basis for such trans-
generational   instability  and  the  mechanism(s)
that   trigger  and/or  release  these  epiallelic  states
will  be  of  great  importance  for  future  studies.
References  and  Notes
1.   J.  A.  Law,  S.  E.  Jacobsen,  Nat.  Rev.  Genet.  11,  204  (2010).
2.   S.   J.   Cokus  et  al.,   Nature  452,  215  (2008).
3.   R.   Lister  et  al.,   Cell   133,  523  (2008).
4.   X.   Zhang  et  al.,   Cell   126,  1189  (2006).
5.   D.   Zilberman,   M.   Gehring,   R.   K.   Tran,  T.   Ballinger,
S.   Henikoff,   Nat.  Genet.   39,  61  (2007).
6.   S.   W.-L.   Chan  et  al.,   Science  303,  1336  (2004).
7.   J. Paszkowski, U. Grossniklaus, Curr. Opin. Plant Biol. 14,
195  (2011).
8.   E.   J.   Richards,   Nat.   Rev.   Genet.   7,  395  (2006).
9.   K.  Shibuya,  S.  Fukushima,  H.  Takatsuji,  Proc.  Natl.  Acad.
Sci.   U.S.A.   106,  1660  (2009).
10.   P.   Cubas,   C.  Vincent,   E.  Coen,   Nature  401,   157  (1999).
11.   K.   Manning  et  al.,   Nat.   Genet.   38,  948  (2006).
12.   A.   J.   Thompson  et  al.,   Plant  Physiol.   120,  383  (1999).
13.   M.   W.   Vaughn  et  al.,   PLoS  Biol.   5,  e174  (2007).
14.   F.   Johannes  et  al.,   PLoS  Genet.   5,  e1000530  (2009).
15.   F.   K.   Teixeira  et  al.,   Science  323,  1600  (2009);
10.1126/science.1165313.
16.   A.   Vongs,   T.   Kakutani,   R.   A.   Martienssen,   E.   J.   Richards,
Science  260,   1926  (1993).
17.   R.   G.   Shaw,   D.   L.   Byers,   E.   Darmo,   Genetics  155,  369
(2000).
18.   S.   Ossowski   et  al.,   Science  327,   92  (2010).
19.   Additional  experiments  and  descriptions  of methods  used
to  support  our  conclusions  are  presented  as  supporting
material   on  Science  Online.
20.   C. M. Nievergelt et al., Am. J. Med. Genet. B. Neuropsychiatr.
Genet. 141B, 234 (2006).
21.   M.   A.   Zapala,   N.   J.   Schork,   Proc.   Natl.   Acad.   Sci.   U.S.A.
103,  19430  (2006).
22.   R.   K.   Chodavarapu  et  al.,   Nature  466,   388  (2010).
23.   J.   Liu,   Y.   He,   R.   Amasino,  X.   Chen,   Genes  Dev.   18,
2873  (2004).
24.   J.   Bender,   G.  R.   Fink,   Cell   83,  725  (1995).
25.   S.   Melquist,   B.  Luff,   J.   Bender,   Genetics  153,  4017
(1999).
26.   S.   E.  Jacobsen,  E.  M.   Meyerowitz,   Science  277,  1100
(1997).
27.   H.   Saze,   T.   Kakutani,   EMBO  J.   26,  3641  (2007).
28.   W.   J.   Soppe  et  al.,   Mol.   Cell   6,  791  (2000).
29.   R.   A.   Mosher  et  al.,   Nature  460,  283  (2009).
30.   R.   K.   Slotkin  et  al.,   Cell   136,  461  (2009).
Acknowledgments:   We  thank  M.  White,   R.   Lister,   M.   Galli,
and  R.   Amasino  for  discussions;   R.   Shaw  and  E.   Darmo
for  seeds;   J.   Nery  for  sequencing  operations;   and
M.  Axtell  for  Southern  blot  protocol.  R.J.S.  was  supported
by  an  NIH  National   Research  Service  Award  postdoctoral
fellowship  (F32-HG004830).   M.D.S.   was  supported  by
a  NSF  Integrative  Graduate  Education  and  Research
Traineeship  grant  (DGE-0504645).  M.G.L.  was  supported
by  an  European  Union  Framework  Programme  7
Marie  Curie  International   Outgoing  Fellowship
(project  252475).   O.L.   and  N.J.S.   are  supported  by
NIH/National   Center  for  Research  Resources  grant
number  UL1  RR025774.   This  work  was  supported  by
the  Mary  K.   Chapman  Foundation,   the  NSF  (grants
MCB-0929402  and  MCB1122246),   the  Howard  Hughes
Medical   Institute,   and  the  Gordon  and  Betty  Moore
Foundation  (GBMF)  to  J.R.E.   J.R.E.   is  a  HHMIGBMF
Investigator.  Analyzed  data  sets  can  be  viewed
at  http://neomorph.salk.edu/30_generations/browser.
html.   Sequence  data  can  be  downloaded  from  National
Center  for  Biotechnology  Information  Sequence  Read
Archive  (SRA035939).  Correspondence  and  requests  for
materials should be addressed to J.R.E. (ecker@salk.edu).
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/science.1212959/DC1
Materials  and  Methods
SOM  Text
Figs.   S1  to  S11
Tables  S1  to  S16
References
22  August  2011;   accepted  7  September  2011
Published  online  15  September  2011;
10.1126/science.1212959
Computation-Guided  Backbone
Grafting  of  a  Discontinuous  Motif
onto  a  Protein  Scaffold
Mihai  L.   Azoitei,
1
*  Bruno  E.  Correia,
1,2
*  Yih-En  Andrew  Ban,
1
  Chris  Carrico,
1,3
Oleksandr  Kalyuzhniy,
1
Lei  Chen,
4
Alexandria  Schroeter,
1
Po-Ssu  Huang,
1
Jason  S.  McLellan,
4
Peter  D.  Kwong,
4
David  Baker,
1,5
Roland  K.  Strong,
3
William  R.  Schief
1,6,7
The  ability  of  electrospray  to  propel  large  viruses  into  a  mass  spectrometer  is  established  and  is
rationalized by analogy to the atmospheric transmission of the common cold. Much less clear is the
fate  of  membrane-embedded  molecular  machines  in  the  gas  phase.  Here  we  show  that  rotary
adenosine triphosphatases (ATPases)/synthases from  Thermus thermophilus and  Enterococcus  hirae
can  be  maintained  intact  with  membrane  and  soluble  subunit  interactions  preserved  in  vacuum.
Mass  spectra  reveal  subunit  stoichiometries  and  the  identity  of  tightly  bound  lipids  within  the
membrane rotors. Moreover, subcomplexes formed in solution and gas phases reveal the regulatory
effects  of  nucleotide  binding  on  both  ATP  hydrolysis  and  proton  translocation.  Consequently,  we
can  link  specific  lipid  and  nucleotide  binding  with  distinct  regulatory  roles.
R
otary  ATPases/synthases  are  membrane-
associated  molecular  machines  that   per-
form biological energy conversion. Both
V-type  and  F-type  complexes  consist  of  two  re-
versible  motors:  the  ion  pump/turbine  in  V
O
/F
O
and  the  chemical  motor/generator  in  V
1
/F
1
.  The
mode  of  operation  is  influenced  by  the  ratio  of
the  two  fuels  (protons:ATP)   that   drive  the  two
motors. (13). The membrane-embedded V
O
/F
O
domain mediates the movement of Na
+
or pro-
tons  across  the  membrane,  whereas  V
1
/F
1
  do-
mains  interact   with  nucleotides  and  inorganic
phosphate either to produce or consume ATP in
the case of the eukaryotic F- and V-type families,
respectively.   Eubacteria  and  archaea  typically
have  only  one  type  of  rotary  ATPase/synthase
for both functions. Most bacteria have complexes
of  the  F-type,  but  some  bacteria  and  all  known
archaea  have  complexes  closely  related  to  eu-
karyotic V-type ATPases [also known as A-type
ATPases/synthases (4)]. Whether of F- or V-type,
the  physiological   function  of   most   prokaryotic
complexes is ATP synthesis; however, many have
evolved  regulatory  functions  that  allow  reversal
into ATP-driven proton pumps if required.
F
1
-F
O
, and V
1
-V
O
, are mechanically coupled
by  a  central  rotating  shaft  and  held  together  by
peripheral stalks (Fig. 1). Structural details derive
from  isolated  subcomplexes  of  F
1
  and  V
1
  (57)
and from membrane embedded proteolipid rings
of various species (811). Despite this wealth of
structural information, no high-resolution struc-
tures of any intact rotary ATPases/synthases have
been reported. Thus, regulatory allosteric changes
that involve both the soluble head and the mem-
brane  sector  are  lost.   In  addition  heterogeneous
interactions  with  lipids  and  nucleotides  are  dif-
ficult to observe with existing structural biology
approaches.
We  show  using  electrospray  mass  spectrom-
etry  (MS)  that  rotary  ATPases/synthases  from
Thermus   thermophilus  (TtATPase)   and  Entero-
coccus hirae (EhATPase) can remain intact in the
gas phase. Previously, composite models were as-
sembled of the intact TtATPase by low-resolution
electron  microscopy  (EM)   data  in  combination
with high-resolution x-ray structures of subunits
(12),   whereas  the  first   cryo-EM  data  revealed
views of the entire membrane-embedded region
(13). We compared the MS of the two complexes,
the  TtATPase  with  that   of  the  less  well   charac-
terized  EhATPase. Current models suggest that
the  EhATPase has only one peripheral stalk (14),
and  the  stoichiometry  of  the  K  subunits  in  the
membrane  ring  was  determined  as  seven  from
EM (15) and 10 from x-ray analysis (8).
TtATPase was purified as described (16) with
dodecyl maltoside (DDM) for solubilization, be-
cause under these conditions the complex is most
stable and does not formaggregates. The complex
was introduced into a mass spectrometer modified
for high-mass complexes (17). Well-resolved charge
states were assigned to the intact particle consist-
ing  of   26  subunits   and  nine  different   proteins
(Fig. 1A). An experimentally determined mass of
659,202 (T131) dalton corresponds to that calcu-
lated for the intact complex, on the basis of subunit
masses determined by MS(table S1), plus addition-
al mass due to incomplete desolvation, and lipid
and nucleotide binding (fig. S1). Gas-phase ac-
tivation is necessary to release the complex from
its detergent micelle (18,  19), giving rise to peaks
at   higher  mass/charge  ratio  (m/z)  than  the  intact
1
Department  of Chemistry,  Physical  and Theoretical  Chem-
istry  Laboratory, University of Oxford, Oxford OX1 3QZ, UK.
2
Department  of  Chemistry,  Lensfield  Road,  University  of  Cam-
bridge,  Cambridge  CB2  1EW,  UK.
  3
Department  of  Physiol-
ogy,   Pontificia  Universidad  Catlica  de  Chile,   Alameda  340,
Santiago,   Chile.
  4
Department  of  Chemistry,  Graduate  School
of Science, Chiba University, 1-33 Yayoi-cho, Inage, Chiba 263-
8522, Japan.
  5
Department of Chemistry,  University  of Texas
at El Paso, El Paso, TX 79968, USA.
  6
The Victor Chang Cardiac
Research Institute, Lowy Packer Building, 405 Liverpool Street,
Darlinghurst NSW 2010, Australia.
  7
Faculty of Medicine, Uni-
versity  of  New  South  Wales,  Sydney  2052,  Australia.
*These  authors  contributed  equally  to  this  work.
To  whom  correspondence   should  be   addressed.   E-mail:
carol.robinson@chem.ox.ac.uk
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 380
REPORTS
complex,   formed  by  unfolding  and  dissociation
of highly charged subunits, predominantly sub-
units  E,   G,   and  I   (20)   (fig.   S2).   At   lower   m/z,
charge  states   are  assigned  to  the  membranous
subcomplex  V
O
  (ICL
12
),  their  bimodal  distribu-
tion implying  that  they  are formed both in solu-
tion  and  gas  phases.  The  corresponding  soluble
V
1
 complex is also observed, confirming that un-
der  these  solution  conditions  a  proportion  of  the
complex dissociates spontaneously (21) (fig. S3).
Using  similar  experimental  parameters,  we
recorded a spectrumfor the EhATPase isolated in
DDM, where its functional activity has been es-
tablished  previously  (22,   23).  The  membrane-
embedded rotor for this complex is larger because
each Ksubunit contains four transmembrane heli-
ces as compared with two for the corresponding
L subunits from TtATPase. Under conditions in
which  the  complex  emerges  from  the  micelle
surviving intact, the spectrumis not well resolved
(fig. S4). Increases in activation energy lead to
better  desolvation and  also appearance  of sub-
complexes  in  which  either  the  membrane  ring
remains  but the peripheral  stalks  and subunit I
have dissociated, or the stalk subunits are attached
but the membrane region is disrupted (Fig. 1B
and fig. S5). The number of peripheral stalks was
determined as two and the stoichiometry in the
K ring as 10 (175 kD) (fig. S6).
The  lipid  components  in  the  K
10
  ring  were
identified as a series of negatively charged cardio-
lipins (figs. S2 and S7 and table S2). The stoi-
chiometry of lipid binding was determined as 10
from the mass of the membrane ring. We iden-
tified six cardiolipin isomers and, from quanti-
tative analysis and measurement of the protein
concentration,   deduce  specific  binding  of  one
lipid per subunit [Eh Ksubunit 1: 1.2 T 0.1 cardio-
lipins (fig. S8)]. Previously, the lipids were lo-
cated based on the atomic structure of the isolated
K
10
 ring, in which peaks of positive density were
attributed  to  20  bifurcated  phosphatidylglycerol
lipids (8). We docked 10 negatively charged sym-
metric cardiolipins inside the K
10
 ring, proximal
to  the  conserved  Lys
32
.  The  four  hydrophobic
chains are positioned with two chains emanating
fromboth sides of the polar head, thus providing a
hydrophobic liningtothe inside of the ring (Fig. 2A).
For  the  TtATPase L
12
 ring, we identified the
bound lipid as phosphatidylethanolamine  (PE)
(Fig. 2 and fig. S9). Unexpectedly, dissociated
L subunits were observed either with bound PE
lipid (holo) or without lipid (apo) after tandem
MS of a subcomplex containing the membrane
subunits  and  peripheral  stalks  (Fig.  2).  Before
disruption, the mass of the subcomplex is con-
sistent with binding of six lipids. This means that
apo and  holo subunits coexist within the same
complex. We confirmed this observation by quan-
tifying the protein:lipid ratio as one L subunit:
0.55  T  0.1  PE  (i.e.,  one  PE  lipid  per  L  subunit
dimer) (fig. S10). Six equivalent binding sites for
lipids in protein dimers in a 12-membered ring
imply a sixfold symmetrical state. Previously, EM
studies of the same preparation of the  TtATPase
revealed a sixfold symmetric membrane-embedded
ring (Fig. 2 and fig. S11) (16). Both sets of data
are  consistent  with  close  packing  of  two  neigh-
boring  subunits,  forming  six  dimers  each  with
four  transmembrane  helices  (TMHs),  thus  emu-
lating  the  arrangement  of  C  subunits  in  eukary-
otic V-ATPases in which gene duplication has led
to four TMHs per subunit (24,  25). From model-
ing,   we  find  that   a  rotation  of   the  dimers  by
about   60  relative  to  their  original   orientation
in the ring  effectively  locks  six  Glu
63
residues
in an occluded position, preserving lipid binding
at the dimer interface. Proton transfer can occur at
the remaining six active glutamates [Fig. 2, (i) to
(iii)];  consequently,  the  proton:ATP  ratio  for  the
rotary enzyme is effectively halved.
A
B
L
K
52+
25+
32+
G G E
E
19+
45+
36+
G G E
E
-C
-F
-F
- I(EF)
2
r
e
l
a
t
i
v
e
 
i
n
t
e
n
s
i
t
y
 
(
%
)
m/z 10000   15000   20000   25000
100
0
C
D
B
A
G
C
E
F
D
B
A
G
D
B
A
C
E
D
B
A
G
E
F
D
B
A
G
E
D
B
A
G
m/z
100
26+
34+
-G
-E
6000   9000   12000   15000
57+
45+
r
e
l
a
t
i
v
e
 
i
n
t
e
n
s
i
t
y
 
(
%
)
0
26+
L
C
G
D
B
A
F
I
L
C
G
E
D
B
A
F
I
L
C
D
B
A
F
I
L
C
I
B
F
C
D
I
G
E
A
L
C
I
7800 7000
24+
K
E
F
B
A
G
D
K
C
I
Fig. 1. Mass spectra of the intact rotary ATPases from T. thermophilus and E. hirae. (A) Peaks are assigned
to the intact TtATPase complex (stars), loss of the membrane subcomplex (ICL
12
) in solution and gas phases
(dark green and green hexagons, respectively), and dissociation of subunits E and G from the peripheral
stalk (blue circles and squares respectively). (B) For EhATPase, the membrane subcomplex is observed in
contact with the soluble head (green squares). (Inset) Mass spectra of the K ring in aqueous solution.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   381
REPORTS
In contrast to  E.  hirae, which has both F- and
V-type ATPases,  T.  thermophilus  has only one
type of rotary ATPase that operates in both pro-
ton pumping and ATP synthesis modes in vitro
(26). Given that each of the 12 L subunits in the
TtATPase  membrane  ring  contains  only  two
TMHs, alternating between synthesis and pumping
would involve switching the 12-membered ring
from  a  high  proton:ATP  ratio,  primed  for  syn-
thesis (27), into a lower one biased for pumping
(16).   This  latter   scenario  thus  mimics  the  eu-
karyotic  V-type enzyme where gene duplication
has  provided  four   TMHs  each  with  one  active
glutamate.  Consequently,  this  mechanism  for
switching between ATP synthesis and ion-pumping
modes is likely assisted by specific lipid binding
for this dual-function rotary ATPase.
These  different   lipid-binding  patterns  in  the
two rotary ATPases studied here were  found to
be   invariant   between  repeat   preparations   and
different detergent concentrations. Together, they
provide  an  explanation  as  to  how  the  disparate
membrane rings L
12
 and K
10
 (93.6 and 160 kD)
can interact with their respective Csubunits (35.8
and 38.2 kD), which are likely conserved. Lining
with cardiolipin, bound specifically to the inside
of  the  K
10
  ring,  reduces  the  orifice  from  54  to
38 (Fig. 2Aand fig. S12). Similarly, converting
a 12- to a 6-membered ring for TtATPase reduces
the  orifice  from  47  to  39  ,  creating  two  very
similar inner diameters (38 and 39 ) (Fig. 2B).
To assess the role of nucleotides in changing
subunit interactions, we compared spectra for the
TtATPase, with and without addition of 50 mM
ATP. In the presence of ATP, the intact complex
and  membrane-embedded  subcomplex  ICL
12
are the predominant species formed in solution
(Fig. 3A and fig. S13). When ATP is depleted,
loss of subunit B leads to extensive dissociation
of  the  soluble  head.  In  addition,  tandem  MS  of
V
1
in the presence of ATP leads predominantly to
loss of subunit F, with subsequent loss of subunit
A
B
C
D
C H
3
O
O
O
O
P
O
O
NH
3
+
O
-
O H
C H
3
C H
3
O
O
C
O
P
OH
O
O
C H
3
O
O H
C H
O
O
C
O
P
O
O
O H
C H
3
3
O
O H
O H
H
(iii) (ii) (i) (iv)
2000 4000                                   
%
0
100
18000 16000
34+ 35+
36+
8500 8000
3+
4+
2+
3+
4+
5+
6+
2+
12+
11+
12+
10+
C
m/z
Fig.   2.   Lipid  binding  and  its  effect  on  the  membrane  rings.  (Upper  panel)
Predominant lipid molecules, one of the six cardioplipins (left) and phos-
phatidylethanolamine (PE, right), found in intact EhATPase and TtATPase,
respectively.   (Central   panel)  Tandem  MS  of  a  subcomplex  from  TtATPase
[ICL
12
E
2
G
2
F (282 740 daltons)] leads to disruption of the L
12
 ring, releasing
proteolipids L  T PE (red/green circle, 8539 daltons; red circles, 7849 daltons)
and a stripped-complex  ICE
2
G
2
F (blue squares,  184 242 daltons). Atomic
structure of the K
10
 ring (8) of EhATPase with docking of 10 cardioplipins to
show reduction in the inner diameter (A) and after docking subunit C (B).
Models for sixfold symmetry of the L
12
 ring with six PE molecules (green)
(C) and with subunit C (42) (blue) docked into the ring (D). (Lower panel)
schematics of the rotor ring with 12 L subunits each having two TMHs (red
cylinders) and one conserved Glu
63
(yellow) as seen in EM of two-dimensional
crystals of isolated L ring (27) (i). Transformation into a sixfold symmetric ring
[(ii) and (iii)]. (iv) Comparison of the sixfold symmetrical model with EM data
reported previously for the intact TtATPase (iv) (16).
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 382
REPORTS
D  (Fig.  3B).  When  ATP  is  depleted,  however,
loss of subunit D before subunit F becomes pos-
sible,   leaving  a  subcomplex  with  F  interacting
directly with the A
3
B
3
  hexamer. Extension of
F  toward  the  soluble  head  has  been  proposed
previously as a  braking mechanism to prevent
unregulated  consumption  of  ATP  after  in  vivo
dissociation  of  the  head  from  the  base  in  yeast
V-ATPase (28). In line with this proposal, an x-ray
structure and cryo-EM reconstruction of the iso-
lated A
3
B
3
DF complex fromTtATPase and yeast
V-ATPase  respectively,   also  reveal   interactions
of subunit F with the A
3
B
3
 hexamer (7,  29). An
x-ray  structure  of  the  auto-inhibited  F
1
  head  of
the  Escherichia  coli   F-ATPase  showed  interac-
tions  between  the  subunits  analogous  to  F
1
  e
and  b  in  the  soluble  head  (30).  Subjecting  the
E.  coli F
1
 complex to the same tandem MS pro-
cedure  outlined  above  showed  that   subunit   e
makes direct interactions with the soluble head
(fig. S14). The similar MS dissociation patterns
observed in E. coli F-ATPase, in which the braking
mechanism is well established, and in  TtATPase
suggest   an  analogous  mechanism  to  prevent
ATP hydrolysis in the uncoupled V
1
 complex of
TtATPase.
We  observed  further  sensitivity  of  TtATPase
to  low  ATP  concentrations,  notably  loss  of  sub-
unit I fromICL
12
to formCL
12
(Fig. 3A). Expan-
sion of the peaks assigned to ICL
12
 is consistent
with  binding  of  up  to  six  lipids  and  up  to  two
nucleotides (ATP or ADP) (fig. S15). This agrees
with proposals that a eukaryotic functional equiv-
alent of subunit I senses cellular nucleotide levels
by binding selectively to ADP and undergoing
conformational change (31). To investigate this
conformational  change, we applied ion mobility
MS (IM-MS) (32) to the intact  TtATPase, ICL
12
,
and CL
12
 subcomplexes
.
 Because ions with mul-
tiple  conformations  result   in  broad  arrival-time
distributions  (ATDs),  we  conclude  that  the  rela-
tively compact ATDs for both the intact ATPase
and CL
12
 are consistent  with one predominant
conformation (fig. S16 and tables S3 and S4). By
contrast,  the  ATDs  for  the  ICL
12
  complex  are
much broader than those of the intact TtATPase
and CL
12
, consistent with multiple conformations
of  subunit  I  in  the  isolated  V
O
  complex  (Fig.  4
and table  S4). The lack of conformational het-
erogeneity in the intact complex is rationalized
by the  tethering of subunit I by forces exerted
by the peripheral  stalks  (subunits  E and G), as
suggested  recently  (13).  Once  released  from  the
intact complex, subunit I in V
O
is not constrained,
and  flexibility  of   the  hinge  domain,   located
between the soluble and transmembrane domains,
likely leads to its conformational heterogeneity.
I
D
6000   8000   10000   12000
I
n
t
e
n
s
i
t
y
 
(
%
)
L
C
G
E
A
F
C
I
L
C
B
F
D
2000   10000   14000   18000   22000
37+
38+
26+
31+
30+
17+
17+
19+
7+
15+
L3+
L3+
7+
15+
m/z
ADP
ATP
ATP
ADP
D
B
A
F
D
A
F
B
D
B
A
F
D
A
B
A
F
B
A
B
F
D
D
B
A
F
D
B
A
F
A
B
D
D
 14+
 13+
 19+
 7+
 12+
 7+
D
 FF
L
C
L
C
I
ATP
ADP
+
F
56+
56+
26+
25+
19+
L
I
I   L
C
G
E
D
A
F
A   B
B
Fig.   3.   Nucleotide  binding  and  its  effects  on  intact   TtATPase  and  the
membrane-embedded  and  soluble  head  complexes.   (A)   Depletion  of  ATP
leads to dissociation of the B subunit fromthe head and subunit I fromICL
12
.
(B) Tandem MS of the soluble head (A
3
B
3
DF) reveals sequential loss of sub-
units F and D in the presence of 50  mM ATP. In TtATPase solutions containing
50  mM  ADP,  two  conformations  of  subunit  F  are  evident  from  the  bimodal
distribution of charge states formed for the V
1
 stripped of F (D7+ and  D12+)
together  with  a  direct   loss  of   subunit   D.   The  D7+  series  is  similar  to  that
formed from the ATP-bound complex. The  D12+ series is consistent with an
extended  conformation  of  subunit  F.  (Inset)  Schematic  representation  of  ef-
fects of ATP/ADP on the membrane ICL
12
 complex and the movement of an
extended subunit F in the A
3
B
3
DF complex.
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   383
REPORTS
The soluble domain of I in EM density maps
of  the  intact   TtATPase  is  at   90  to  the  proton
channel (12, 13). Our IMdata for the V
O
complex,
based on modeling of the ICL
12
 and CL
12
 com-
plexes  (fig.  S17),  are  consistent  with  a  range  of
conformational  states  with  angles  from  90  to
135  (fig.   S18).  We  propose,   therefore,   that  the
conformational dynamics demonstrated here, to-
gether  with  preferential   binding  of  ADP  to  the
proposed site near the hinge region (31), destabi-
lize interactions between I and CL
12
as evidenced
by  the  facile  loss  of  subunit  I  under  low-ATP
conditions.
Given  that   cellular   nucleotide   levels   likely
affect   proton  translocation  in  the  isolated  V
O
complex, it might also be anticipated that changes
in the proton gradient would induce similar reg-
ulatory  effects.  To  test  this  hypothesis,  we  in-
creased the pHof the ATPase-containing solution
to  mimic  reduction  of  the  proton  concentration.
Mass  spectra  of  the  TtATPase  incubated  at   pH
9.0  led  to  subcomplexes  formed  by  loss  of  IGE
(fig.   S19).   This   observation,   together   with  the
dissociation of subunit I from V
O
, suggests a reg-
ulatory  role  for  subunit  I,  sensing  both  proton
and  ATP  concentrations.  Previous  proposals  in-
voked a locking together of the membrane por-
tion of subunit I with the CL
12
 membrane ring,
preventing relative movement and hence explain-
ing  the  absence  of  passive  H
+
translocation  in
isolated V
O
 (33, 34). Because we observe facile
loss  of  subunit  I  under  both  lowH
+
concentra-
tion ([H
+
]) and low-[ATP] conditions, and given
the  lack  of  extensive  interactions  between  I  and
the  membrane  ring  observed  in  cryo-EM  data
(13), our results point to a mechanism in which
subunit I moves away from the ring, and the re-
sulting gap could then be sealed with membrane
lipids (Fig. 4D).
Our results showthat lipids with two and four
hydrophobic chains associate with subunits with
two and four TMHssubunits L and K, respec-
tively. In both ATPases, the lipids identified in
situ  are  not  the most  prevalent  ones  in  the  cell
(35,  36), implying that lipids are selected from
the  available  pool   for  specific  structural   roles
and metabolic regulation. This further supports
the  proposal   that   membrane  proteins  possess
specific  lipid  binding  sites  (37)   and  demon-
strates the ability of lipids to fine tune subunit
interactions  by  defining  the  conformations  and
inner  dimensions  of  the  membrane  rings.   Our
nucleotide-binding experiments show that a de-
crease in cellular ATP concentrations is sensed
by V
1
, not only with the movement of subunit
F but also with changes in interactions at the A:B
interface. Unexpectedly, V
O
 is also sensitive to
low [ATP] and [H
+
], both of which promote dis-
placement of subunit I. We suggest that membrane
lipids subsequently seal the proton-conducting
channel. Consequently, both ATP and proton/ion
gradients  are  conserved  when  reversible  disso-
ciation takes place in vivo.
The   existence   of   intact   rotary   ATPases/
synthases   in  vacuum  has   been  demonstrated
previously  with  LILBID  MS  (38,   39).  At  its  cur-
rent   resolution,   however,   it   is  not   possible  to
identify bound lipids or nucleotides or to probe
their effects on subunit interactions. Moreover,
previous   ES-MS  experiments   produced  well-
resolved mass spectra for the V
1
domain (40, 41),
but lack of an intact V
O
domain, or any interactions
between V
1
 and V
O
, is attributed to dissociation
of the complex in the absence of the protective
micelle  (18,   19).  By  contrast,  the  ES  approach
used  here  enables  interrogation  of  subunit  inter-
actions  within  intact   rotary  ATPase/synthases
and allows us to probe the synergistic effects of
lipid and nucleotide binding.
References  and  Notes
1.   K.   C.   Jefferies,   D.   J.   Cipriano,   M.  Forgac,   Arch.   Biochem.
Biophys.   476,  33  (2008).
2.   C. von Ballmoos,  A. Wiedenmann, P. Dimroth, Annu. Rev.
Biochem.   78,  649  (2009).
5000 6000 7000 8000 9000
21+
5
20
15
D
r
i
f
t
 
t
i
m
e
 
(
m
s
)
10
7
22
17
D
r
i
f
t
 
t
i
m
e
 
(
m
s
)
12
m/z
A
25+
ADP
ATP
E
r
H
+
D
no ATP / with ADP with ATP
membrane
   lipids
Drift time (ms)
5 20 35
%
0
100
10.62
10.97
11.49
B
Drift time (ms)
21+
22+
23+
%
0
100
16.05
16.91
17.94
19.48
5 20 35
24+
25+
26+
C
L
C
L
C
I
Fig. 4. Conformational heterogeneity and dissociation of subunit I fromICL
12
implies  a  mechanism  for  closing  the H
+
channel.  (A)  IM-MS  of  the  trans-
membrane ICL
12
 and CL
12
 complexes formed in solution from intact TtATPase.
Charge states used for IM measurement are labeled gray and red (B and C).
Broader arrival-time distributions for ICL
12
 than for CL
12
 are consistent with
conformational heterogenity in subunit I. (D) Possible mechanism to  close
the  H
+
channel  after  lateral  movement  of subunit I  within the  membrane.
Surrounding  lipids  effectively  block  the  channel.   The  direction  of   proton
pumping (green) and rotation of the ring (yellow) for ATP hydrolysis, as seen
fromthe top (site of interaction with V
1
). (E) Coarse-grained and atomic model
of  the  ICL
12
  complex  generated  according  to  IM  restraints  and  homology
modeling  (see  supplementary  methods).  The  proposed  nucleotide  binding
area in the hinge region of I (orange) and Glu
63
:Arg
563
from subunits L and I
are shown in yellow and green, respectively.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 384
REPORTS
3.   S. P. Muench, J. Trinick, M. A. Harrison, Quat. Rev. Biophys.
44,  311  (2011).
4.   V.   Mller,  G.  Grber,  Cell.  Mol.  Life  Sci.  60,  474  (2003).
5.   J. P. Abrahams, A. G. Leslie, R. Lutter, J. E. Walker, Nature
370,  621  (1994).
6.   K.   Okazaki,   S.  Takada,   Structure  19,  588  (2011).
7.   N.  Numoto,  Y.  Hasegawa,  K.  Takeda,  K.  Miki,  EMBO  Rep.
25,   25  (2009).
8.   T. Murata, I. Yamato, Y. Kakinuma, A. G. Leslie, J. E. Walker,
Science  308,  654  (2005).
9.   T.   Meier,  P.   Polzer,   K.   Diederichs,   W.   Welte,   P.   Dimroth,
Science  308,   659  (2005).
10.   A.   Dautant,   J.   Velours,   M.  F.   Giraud,   J.   Biol.   Chem.  285,
29502  (2010).
11.   I.  N.  Watt,  M.  G.  Montgomery,  M.  J.  Runswick,  A.  G.  Leslie,
J.  E.  Walker,  Proc.  Natl.  Acad.  Sci.  U.S.A.  107,  16823
(2010).
12.   L.  K.   Lee,  A.   G.   Stewart,   M.   Donohoe,   R.   A.   Bernal,
D.   Stock,   Nat.   Struct.   Mol.   Biol.   17,  373  (2010).
13.   W.   C.  Lau,   J.   L.  Rubinstein,   Proc.   Natl.   Acad.   Sci.   U.S.A.
107,  1367  (2010).
14.   M.  Yamamoto  et  al.,   J.   Biol.   Chem.   283,   19422  (2008).
15.   T.  Murata  et  al.,   J.   Biol.   Chem.  278,   21162  (2003).
16.   R.   A.   Bernal,   D.  Stock,  Structure  12,  1789  (2004).
17.   H.  Hernndez,  C.  V.  Robinson,  Nat.  Protoc.  2,  715  (2007).
18.   N.  P.  Barrera,   N.  Di   Bartolo,   P.  J.  Booth,   C.  V.  Robinson,
Science  321,   243  (2008).
19.   N.  P.   Barrera  et  al.,   Nat.   Methods  6,  585  (2009).
20.   J. L. Benesch, C. V. Robinson, Curr. Opin. Struct. Biol. 16,
245  (2006).
21.   K.   Yokoyama  et  al.,   J.   Biol.   Chem.   278,   42686  (2003).
22.   K.   Takase  et  al.,   J.   Biol.   Chem.   269,   11037  (1994).
23.   T. Murata, K. Takase, I. Yamato, K. Igarashi, Y. Kakinuma,
J.   Biochem.   125,   414  (1999).
24.   M.   Mandel   et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.  85,   5521
(1988).
25.   D.   K.   Clare  et  al.,   Structure  14,  1149  (2006).
26.   K.   Yokoyama  et   al.,   J.   Biol.   Chem.   275,   13955
(2000).
27.   M.   Toei   et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.  104,  20256
(2007).
28.   P.   M.   Kane,   A.   M.   Smardon,   J.   Bioenerg.   Biomembr.  35,
313  (2003).
29.   Z.   L.   Hildenbrand,   S.  K.   Molugu,   D.   Stock,   R.   A.   Bernal,
PLoS  ONE  5,   e12588  (2010).
30.   G.   Cingolani,   T.  M.   Duncan,  Nat.   Struct.   Mol.   Biol.   18,
701  (2011).
31.   A.   Armbrster  et  al.,   FEBS  Lett.   579,  1961  (2005).
32.   C.   Uetrecht,   R.   J.   Rose,   E.   van  Duijn,   K.   Lorenzen,
A.   J.   Heck,   Chem.   Soc.   Rev.   39,  1633  (2010).
33.   J.  Zhang,  M.  Myers,  M.  Forgac,  J.  Biol.  Chem.  267,  9773
(1992).
34.   C.   Beltrn,  N.   Nelson,   Acta  Physiol.   Scand.   Suppl.   607,
41  (1992).
35.   D.   Carson,   R.   A.   Pieringer,   L.   Daneo-Moore,   Biochim.
Biophys.   Acta  575,  225  (1979).
36.   P. H. Ray, D. C. White, T. D. Brock, J. Bacteriol. 108, 227 (1971).
37.   C.   Hunte,   S.  Richers,   Curr.   Opin.   Struct.   Biol.   18,  406
(2008).
38.   T.   Meier  et  al.,   Mol.   Microbiol.   65,  1181  (2007).
39.   J.   Hoffmann  et  al.,   Phys.   Chem.   Chem.   Phys.   12,   13375
(2010).
40.   O.   Esteban  et  al.,   J.  Biol.   Chem.   283,  2595  (2008).
41.   N.   Kitagawa,   H.   Mazon,   A.   J.   Heck,   S.  Wilkens,   J.   Biol.
Chem.   283,  3329  (2008).
42.   M.   Iwata  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.   101,   59
(2004).
Acknowledgments:   Funding  from  the  Wellcome  Trust  and
by  the  PROSPECTS  (HEALTHF4-2008-201648)  grant
within  the  Research  Framework  of  the  European  Union
together  with  funding  from  the  Royal   Society  (C.V.R.),
the  Australian  National   Health  and  Medical   Research
Council   grant  573712  (D.S.),   and  the  FONDECYT
1100515  (N.P.B.)  is  acknowledged.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/380/DC1
Materials  and  Methods
Figs.   S1  to  S19
Tables  S1  to  S4
References  (4358)
22  June  2011;   accepted  15  September  2011
10.1126/science.1210148
Cerebellum  Shapes  Hippocampal
Spatial  Code
Christelle  Rochefort,
1
*  Arnaud  Arabo,
1
*  Marion  Andr,
2
  Bruno  Poucet,
2
Etienne  Save,
2
*  Laure  Rondi-Reig
1
*
Spatial  representation  is  an  active  process  that  requires  complex  multimodal  integration  from  a
large  interacting  network  of  cortical  and  subcortical  structures.  We  sought  to  determine  the  role
of  cerebellar  protein  kinase  C  (PKC)dependent  plasticity  in  spatial  navigation  by  recording  the
activity  of  hippocampal  place  cells  in  transgenic  L7PKCI  mice  with  selective  disruption  of
PKC-dependent  plasticity  at  parallel  fiberPurkinje  cell  synapses.  Place  cell  properties  were
exclusively  impaired  when  L7PKCI  mice  had  to  rely  on  self-motion  cues.  The  behavioral
consequence  of  such  a  deficit  is  evidenced  here  by  selectively  impaired  navigation  capabilities
during  a  path  integration  task.  Together,  these  results  suggest  that  cerebellar  PKC-dependent
mechanisms are involved in processing self-motion signals essential to the shaping of hippocampal
spatial  representation.
I
t   is   well   established  that   rodents   build  an
internal cognitive map to navigate in their en-
vironment.   A  key  neural   substrate  enabling
such  representation  is  the  hippocampus,   which
contains CA1 and CA3 pyramidal cells described
as place cells. Each place cell fires for a restricted
region (the place field) of the environment (1,  2).
Both  external   cues   and  self-motion  cues   (i.e.,
vestibular,   proprioceptive,   and  optic  flow  cues)
control place cell firing (3, 4), which suggests the
involvement   of  a  large  network  of  cortical   and
subcortical structures interacting with the hippo-
campus for navigation. Determining the function-
al architecture of such a network is thus essential
to  our  understanding  of  how  the  hippocampal
place  cell   code  is  generated.   The  medial   ento-
rhinal cortex, a key relay structure between neo-
cortical areas and the hippocampus, contains grid
cells  with  regularly  spaced  multiple  firing  fields
(5), which integrate self-motion information and
participate in path integration (4,  6,  7).
The  cerebellum  has  also  been  shown  to  be
essential  to  the  processing  of  self-motion  infor-
mation: Cerebellar Purkinje cells respond to vestib-
ular signals by transforming head-centered vestibular
afferent   information  into  Earth-reference  self-
motion and spatial orientation signals (8,  9), and
electrophysiological   investigations   suggest   that
the cerebellumand the hippocampus can be func-
tionally  connected  during  eyeblink  conditioning
(10,   11).   However,   it   is  still   unknown  whether
such an interaction is functionally relevant in nav-
igation,   and  a   mechanism  that   might   underlie
such a process has not been identified.
In  the  transgenic  mouse  strain  L7PKCI,   the
pseudosubstrate protein kinase Cinhibitor (PKCI)
is  selectively  expressed  in  Purkinje  cells  under
the control of the pcp-2 (L7) gene promoter (12).
This results in an impaired long-term depression
(LTD)   at   cerebellar   parallel   fiberPurkinje  cell
synapses. Such a plasticity mechanism has been
proposed to work as an error-based (anti-Hebbian)
learning   process   (13,   14)   during   conditioning
tasks (15) and in optimization of motor response
during navigation (16).
A total of 506 dorsal CA1 hippocampal cells
were  recorded.  A  subset  of  150  place  cells  was
further   analyzed  in  six  L7PKCI   mice  and  five
wild-type littermate control mice. Relative to wild-
type mice, L7PKCI mice had a significantly lower
proportion  of  place  cells  [L7PKCI,   n  =  53/218
(24.3%); wild type, n = 97/288 (33.7%); c
2
= 5.2,
df = 1,  P < 0.025]. Neural activity was sampled
as the mice freely explored a circular arena con-
taining a salient cue (a card with a bottle attached
to  it),   in  standard  sessions  (S1  and  S2)  and  in-
volving cue manipulation in subsequent sessions
(S3 and S4). A last session (S5) similar to ses-
sions  S1 and  S2 was  run  to  determine  whether
we  could  restore  the  initial   firing  pattern  irre-
spective  of  the  changes  in  cell  firing  observed
during the cue manipulation sessions (Fig. 1A) (17).
After  recording  in  the  standard  sessions,  we
used  two  distinct   environmental   manipulations,
cue removal and cue conflict, in which mice are
forced to use self-motion cues. In the cue removal
condition, the arena was in the dark and the cue
1
Neurobiologie des Processus Adaptatifs (UMR 7102), Naviga-
tion,  Memory,  and  Aging  (ENMVI)  Team,  Universit Pierre  et
Marie   CurieCentre   National   de   la   Recherche   Scientifique
(CNRS),   F-75005  Paris,   France.
  2
Laboratory  of  Neurobiology
and Cognition (UMR 6155), Aix Marseille UniversitCNRS, 3
place Victor Hugo, 13331 Marseille, France.
*These  authors  contributed  equally  to  this  work.
Present address: Laboratoire de Psychologie et Neurosciences
de  la  Cognition  et   de  lAffectivit (EA  4306),   Universit de
Rouen,   Facult  des   Sciences,   Place   Emile   Blondel,   76821
Mont-Saint-Aignan Cedex, France.
Present   address:   Department   of   Experimental   Neurophys-
iology, Ruhr University Bochum, Universittsstrasse 150, MABF
01/551, 44801 Bochum, Germany.
To  whom  correspondence   should  be   addressed.   E-mail:
laure.rondi@snv.jussieu.fr
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   385
REPORTS
was removed. A control condition was also per-
formed with the cue still present in darkness (Fig.
1B).   In  the  cue  conflict   condition,   we  used  a
protocol previously developed in rats, in which
the  external cue was rotated 180 in the absence
(hidden   rotation)   or   in   the   presence   (visible
rotation)   of   the   animal,   therefore   producing  a
conflict   between  visual   and  self-motion  infor-
mation  (18).   During  the  conflict,   rats  maintain
place  field  stability  relative  to  the  standard  ses-
sion,   thus  suggesting  the  dominant   use  of   self-
motion cues (18).
The basic firing properties of place cells in the
light condition were unaffected in L7PKCI mice
(table S1). In addition, place field stability (mea-
sured  as  a  correlation  between  two  similar  light
sessions) was higher in L7PKCI mice (0.78 T 0.05)
than in wild-type mice (0.60  T 0.03) (t
146
 = 3.0,
Fig.  1.  The compulsory use of self-motion cues affects hippocampal place cell
properties in L7PKCI mice. (A and B) Schematic diagram of the protocol used to
assess the effect of self-motion stimulation on place cell properties. After two
consecutive standard sessions (S1 and S2), light was turned off (S3 and S4) and
objects were either removed (A) or maintained (B) in the arena. S5 was similar to
S1 and S2. (C and D) Examples of color-coded rate maps showing firing activity
of   wild-type  (WT)   and  L7PKCI   single  CA1  pyramidal   cells  over  the  five  con-
secutive sessions; color coding ranges from blue (silent) to red (peak activity).
Peak firing rates are indicated for each rate map. (E to H) Analysis of place cell
characteristics  shows  that  the  suppression  of  external  cue  inputs  significantly
alters  both  the  mean  field  rate  (E)  and  spatial  coherence  (F)  in  L7PKCI  mice
specifically, whereas the suppression of the visual cue alone has no effect [(G)
and (H)]. (I to L) Place field stability, as measured within (I) or across (J) sessions,
is affected in L7PKCI mice after suppression of all external cues, but not after
suppression of the visual cue alone [(K) and (L)]. *P < 0.05, **P < 0.01, ***P <
0.001 with a Newman-Keuls post hoc analysis. Error bars represent SEM.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 386
REPORTS
P  =  0.003).   In  sharp  contrast,  several  firing  pa-
rameters  were  strongly  affected  in  the  dark  ses-
sions after cue removal in L7PKCI mice (Fig. 1,
C,   E,   and  F,   and  figs.   S1A  and  S2).   The  mean
field rate, peak firing rate, and overall mean firing
rate declined during the dark sessions in L7PKCI
mice but not in wild-type mice (mean field rate,
F
1,39
 = 11.5,  P = 0.002; peak firing rate,  F
1,39
 =
12.1,  P = 0.001; overall mean firing rate,  F
1,39
 =
8.4,   P =  0.006)  (Fig.  1E  and  fig.  S2).  The  field
spatial coherence was also found to be decreased
in  the  dark  (F
1,39
  =  11.2,   P  =  0.002)  (Fig.   1F).
Finally, place field stability in L7PKCI mice was
markedly affected by the dark condition: Where-
as wild-type mice maintained place field stabil-
ity  throughout  the  dark  sessions,  place  cells  of
L7PKCI mice showed a progressive decrease of
within-session stability (F
1,39
= 15.6, P= 0.0003)
as well as between-session stability (F
2,78
 = 6.2,
P= 0.003) (Fig. 1, I and J). These results indicate
that   place  field  stability  in  L7PKCI  mice  grad-
ually  decreased  over  sessions  in  the  dark  (post
hoc analysis;  P < 0.01 between S1-S2 and S2-S3
correlations, P< 0.001 between S1-S2 and S2-S4
correlations) (Fig. 1J).
By  contrast,   place  cell   firing  properties  and
place  field  stability  were  restored  in  session  S5
(fig.   S3).   In  most   instances,   all   simultaneously
recorded  cells  behaved  homogeneously  (i.e.,  all
fields  were  either  stable  or  remapped  together).
The   modification   of   place   cell   properties   of
L7PKCI mice was not due to an impaired explor-
atory  activity in  the  dark,  because  wild-type  and
L7PKCI   mice  displayed  similar   speed  (2.09  T
0.08 cm/s versus 1.97  T 0.05 cm/s,  t
19
 = 1.7,  P >
0.05, t test) and similar traveled distance (14.24 T
0.59  cm  versus  13.10  T  0.35  cm,   t
19
  =  1.4,   P  >
0.05, t test) (Table 1). When the cue was available
in the dark, the firing parameters and place field
stability   were   not   affected   in   L7PKCI   mice
(Fig.  1B  and  fig.  S1B)  (P  >  0.05  for  all  param-
eters analyzed).
These  results  suggest  that  in  the  dark  and  in
the  absence  of  the  cue,  the  place  cell  system  of
L7PKCI mice failed to use self-motion informa-
tion  to  maintain  stable  place  fields.   Consistent
with this finding, the mice were able to maintain
stable  place  fields  when  they  could  update  their
position  by  using  the  cue.   As  a  consequence,
the number of place fields away fromthe object
(>20 cm) was drastically reduced in L7PKCI mice
relative  to  wild-type  mice  [L7PKCI,   n  =  1/16
cells (6%); wild type, n = 20/37 cells (46%); c
2
=
10.67, df = 1,  P = 0.0011]. The relative power
of the hippocampal theta band (5 to 10 Hz) was
similar  in  L7PKCI  and  wild-type  mice  (F1,21  =
1.72,   P  >  0.05)  in  both  light  and  dark  cue  re-
moval conditions (F1,21 = 3.86, P > 0.05), which
suggests  that  alteration  of  path  integration  was
not   caused  by  a  modification  of   theta  rhythm
(fig. S4).
To further investigate the respective influence
of self-motion and external information on spatial
firing  pattern  in  L7PKCI  mice,  we  conducted  a
conflict  condition  protocol  (Fig.  2A).  After  two
standard  sessions,  a  180  hidden  rotation  of  the
cue resulted in similar rotation of the place fields
in  both  wild-type  and  L7PKCI  mice  (Fig.   2,   B
Fig.   2.   Field  locations  are  not  efficiently  controlled  by  self-motion  cues  in
L7PKCI mice. (A) Schematic diagram illustrating the protocol used  to assess
the  effect  on  place  cell  firing  of  a  180  rotation  of  the  cue  in  the  absence
(hidden rotation) or presence (visible rotation) of the mouse in the arena. (B)
Color-coded  rate  maps  showing  firing activity of  WT  and  L7PKCI  single  CA1
pyramidal   cells   over   the  five  consecutive  sessions.   (C  and  D)   Histograms
showing the intersession similarity coefficient score associated to a 0 or 180
field  rotation  after  a  hidden  (C)   or  a  visible  (D)   rotation  of   the  cue.   Field
stability  significantly  decreased  in  L7PKCI  after  a  visible  rotation  of  the  cue
(D).  (E  and  F)  Polar  distribution  of  the  place  field  rotation  angles  after  the
visible rotation in WT mice (E) and L7PKCI mice (F). *P < 0.05, Student t test.
Error bars represent SEM.
Table   1.   General   sensory-motor   abilities   of   WT  and  L7PKCI   mice  in  the  dark  (means   T  SEM).   No
significant differences between WT and L7PKCI mice were revealed by the different sensory-motor tasks
(t test, P > 0.05 for all parameters) assessed in the dark (i.e., using primarily the vestibular system).
Task   Measure
  L7PKCI
(n  =  7)
WT
(n  =  6)
  Mann-Whitney  P
Spontaneous
locomotor  activity  in
the  dark
Speed  (cm/s)   1.97  T  0.05   2.09  T  0.08   0.10
Distance  traveled  (cm)   13.10  T  0.35   14.24  T  0.59   0.09
Rearing  frequency
(number/min)
4.29  T  0.73   6.20  T  0.73   0.18
Dynamic  balance  in
the  dark
Falling  latency  (s)   180   180   
Distance  traveled  (cm)   629  T  77   542  T  51   0.45
Static  balance  in  the  dark   Falling  latency  (s)   144  T  18   105  T  17   0.10
Motor  coordination  in
the  dark  (rotarod)
5  rpm  walking  time  (s)   141  T  21   138  T  12   0.45
10  rpm  walking  time  (s)   141  T  28   157  T  17   0.63
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   387
REPORTS
and  C,  and  fig.  S1C),  indicating that  the cue  ef-
ficiently controlled place cell activity. Visible ro-
tation of the cue was then performed, producing a
conflict between  external and self-motion sen-
sory  information.   During  the  conflict,   63%  of
place cells in wild-type mice maintained their
place field stability relative to the previous ses-
sion  (0   T  30  rotation),   which  suggests  that
the mice resolved the conflict by relying on self-
motion cues (18) (Fig. 2, B, D, and E, and fig.
S1C).   The  distribution  of   place  field  rotation
angles   after   the  visible  rotation  was   therefore
concentrated around the same position (Fig. 2E;
Z =13.53, P< 0.001, Rayleigh test). In contrast, a
majority of place cells in L7PKCI mice exhibited
remapping  at  a  different  location,  leading  to  a
homogeneous  distribution  of   place  field  rota-
tion angles (Fig. 2, B, D, and F; Z = 1.55, P= 0.2,
Rayleigh  test):   30%  of   place  fields  remained
stable, suggesting a control by self-motion cues;
20% exhibited a 180  T 30 rotation, suggesting
a control by the external cue; and the remaining
50%  rotated  at  various  angles.  As  a  result,  field
stability (as measured by intersession  similarity
coefficient   at   a  rotation  angle  of   0)   between
sessions  S4  and  S5  was  significantly  lower   in
L7PKCI  mice  than  in  wild-type  mice  (Fig.  2D;
t
54
  =  2.0,   P  <  0.05).  The  inability  to  maintain
stable place fields in L7PKCI mice strengthens
the idea of a deficit in the use of self-motion cues.
We   next   examined   the   ability   of   L7PKCI
mice   to  navigate   in  the   dark  (i.e.,   using  self-
motion cues). L7PKCI mice were trained to find
an  escape  platform  at  a  constant  location  with  a
constant  departure point in the water maze (Fig.
3A).   Path  optimization  was   analyzed  in  light
and dark conditions (17) (table S3). In the light,
L7PKCI  mice  learned  to  reach  the  platform  as
rapidly and accurately as their control littermates
(Fig. 3, B and C). Both groups increased the use
of direct trajectories across training sessions and
decreased other nonoptimal trajectories (Fig. 3, D
and E). In sharp contrast, navigation performance
in the dark was impaired in L7PKCI mice (Fig. 3,
B  and  C).   Escape  latencies   and  heading  were
significantly  greater   in  L7PKCI   mice  than  in
wild-type  mice  (genotype  effect,   F
1,28
  =  4.98,
P = 0.034, and  F
1,28
 = 9.63,  P = 0.004, respec-
tively),   even  though  there  was  no  difference  in
swimming speed (F
1,28
 = 2.01,  P = 0.2), circling
(F
4,112
  =  0.56,   P  =  0.7)   (fig.   S5),   or   other   be-
havioral parameters that could interfere with nav-
igation  (Table  1  and  table  S2;   P  >  0.05)   (19).
Thus,   assessment   of   navigation  abilities   in  the
dark demonstrates impaired path integration per-
formances in the L7PKCI mice.
The trajectories of the mutant mice were less
efficient than those of their control littermates in
darkness, as highlighted by the differences in the
type  of   trajectory  used  (Fig.   3,   D  and  E).   The
importance of the dark context on the deficit ex-
hibited here by the L7PKCI mice was reinforced
by   the   absence   of   significant   genotype   effect
observed during a control trial that took place in
the  light  condition  during  dark  session  3 (D3T1
in Fig. 3, B and C) (table S3) (17). Accordingly,
comparing  this  trial   with  the  mean  of   the  last
trial (L5) in the light condition revealed no sig-
nificant  differences.  This  indicates  that  the  dis-
turbed trajectories displayed by transgenic mice
in the dark cannot be attributed either to a deficit
in the use of task rules, or to altered motivation.
The fundamental finding of our study is that
mice  lacking  PKC-dependent   cerebellar   LTD
showed disrupted hippocampal place cell proper-
ties and impaired goal-directed navigation in con-
ditions in which self-motion information must be
predominantly  used.  We  previously  suggested  a
role  of PKC-dependent  mechanisms  in the  link-
age  between  the  spatial   context   and  the  motor
response characterized by the animals trajectory
(16,  20). Here, we demonstrate an additional and
complementary  role  of  PKC-dependent  cerebel-
lar  LTD  in  self-motionbased  hippocampal  rep-
resentation  and  path  integration.   Although  the
cerebellumis classically viewed as a motor struc-
ture,   a  growing  body  of  evidence  indicates  that
cerebellar   circuitry  is   well   suited  to  act   as   an
adaptive filter of sensory information (2123). In
particular,   vestibular   information   is   combined
with  proprioceptive  inputs  in  the  cerebellar  fas-
tigial   nucleus   to   generate   appropriate   internal
estimates of the animals self-motion (24). In ad-
dition,  cerebellar  Purkinje  cells  from  lobules  IX
and X transform vestibular head-centered signals
into  self-motion  and  spatial   orientation  signals
relative  to  the  external  world  (8,   9).  It  thus  ap-
pears  that,   beyond  its  role  in  motor  adaptation
during navigation (16,  20), cerebellar LTD con-
tributes  to  the  representation  of  the  relation  of
the body to the external world, thereby shaping
hippocampal spatial representation.
Recent  data  show  a  clear  contribution  of  the
vestibular systemto hippocampal-dependent spa-
tial memory (25, 26) as well as to spatial firing of
Fig.   3.   Inactivation  of  PKC-dependent  cerebellar  LTD  deteriorates  path  integration. (A)  Design  of  the
experimental space developed to evaluate navigation abilities using self-motion cues. (B and C) Quan-
tification  of  escape  latencies  (B)  and  heading  (C)  in  WT  and  L7PKCI  mice  during  both  light  and  dark
conditions. In the light condition, WT and L7PKCI mice improved their performances significantly over
sessions  without  genotype effect.  In  the  dark  condition, both  groups improved  their  performance  over
time, but the performance of LKPCI mice was significantly poorer than that of their control littermates. (D
and E) Swim path analyses during both light and dark conditions. The direct trajectory was significantly
impaired in L7PKCI mice during the dark condition (D). L7PKCI mice cannot perform optimal trajectories
during path integration, as highlighted by the differences between WT and L7PKCI mice in the type of
trajectory used in the dark but not in the light condition (E). The P values indicated in (B) to (D) correspond
to the genotype effect. *P < 0.05 with Newman-Keuls post hoc analysis. Error bars represent SEM.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 388
REPORTS
hippocampal   neurons  (27).   However,   examina-
tion of the vestibular-associated motor activity of
L7PKCI  mice  in  both  light  and  dark  conditions
revealed  no  deficit.   Our   data  do  not   suggest   a
vestibular   implication  underlying  the   observed
alterations  of  place  cell  firing  and  navigation  in
L7PCKI mice. Rather, they demonstrate that cer-
ebellar  LTD  is  also  involved  in  processing  self-
motion  cues.   The   cerebellum  may  therefore
contribute  to  two  major   circuits  crucial   for   the
representation  of  space  in  the  hippocampal  sys-
tem.  The  first  is  the  retrosplenial  cortex,  which
is closely associated with vestibular function (27).
The second is the parietal cortex, which integrates
self-motion and external information and receives
input   from  the  deep  cerebellar   nuclei   (28,   29).
Our study demonstrates the crucial role of PKC-
dependent cerebellar LTD in the preprocessing of
self-motion information required for optimal hip-
pocampal representation. This process appears to
be essential for path integration.
References  and  Notes
1.   H.   Eichenbaum,   Curr.   Biol.   10,  R785  (2000).
2.   J.   OKeefe,   L.   Nadel,   The  Hippocampus  as  a  Cognitive
Map  (Clarendon,   Oxford,   1978).
3.   P. J. Best, A. M. White, A. Minai, Annu. Rev. Neurosci. 24,
459  (2001).
4.   K.   J.   Jeffery,   Hippocampus  17,  775  (2007).
5.   T.  Hafting,  M.  Fyhn,  S.  Molden,  M.  B.  Moser,  E.  I.  Moser,
Nature  436,  801  (2005).
6.   B.  L.  McNaughton,  F.  P.  Battaglia,  O.  Jensen,  E.  I.  Moser,
M.   B.   Moser,   Nat.   Rev.   Neurosci.   7,  663  (2006).
7.   F.   Sargolini   et  al.,   Science  312,   758  (2006).
8.   T.   A.   Yakusheva  et  al.,   Neuron  54,   973  (2007).
9.   D.   E.   Angelaki,   T.   A.   Yakusheva,   A.   M.   Green,
J.  D.  Dickman,  P.  M.  Blazquez,  Cerebellum  9,  174  (2010).
10.   L.  C.  Hoffmann,   S.  D.  Berry,  Proc.  Natl.  Acad.  Sci.  U.S.A.
106,  21371  (2009).
11.   J.   Wikgren,  M.   S.   Nokia,   M.   Penttonen,   Neuroscience
165,  1538  (2010).
12.   C.   I.   De  Zeeuw  et  al.,   Neuron  20,   495  (1998).
13.   J.   S.   Albus,   Math.   Biosci.   10,  25  (1971).
14.   D.   Marr,   J.   Physiol.   202,  437  (1969).
15.   M.   Ito,   M.   Kano,   Neurosci.   Lett.   33,   253  (1982).
16.   E.   Burguire  et  al.,   Nat.   Neurosci.   8,   1292  (2005).
17.   See  supporting  material   on  Science  Online.
18.   A.   Rotenberg,  R.   U.   Muller,   Philos.   Trans.   R.   Soc.
London  Ser.   B  352,  1505  (1997).
19.   L.   Rondi-Reig  et  al.,   Neuroscience  104,   207  (2001).
20.   E.   Burguire,   A.   Arabo,   F.   Jarlier,   C.   I.   De  Zeeuw,
L.   Rondi-Reig,   J.   Neurosci.   30,  13265  (2010).
21.   S.   Pasalar,   A.   V.   Roitman,   W.   K.   Durfee,   T.   J.   Ebner,
Nat.   Neurosci.   9,  1404  (2006).
22.   C. C. Bell, V. Han, N. B. Sawtell, Annu. Rev. Neurosci. 31,
1  (2008).
23.   P.   Dean,   J.   Porrill,   C.   F.   Ekerot,   H.   Jrntell,
Nat.   Rev.   Neurosci.   11,   30  (2010).
24.   J.   X.   Brooks,   K.   E.   Cullen,   J.   Neurosci.   29,   10499
(2009).
25.   Y.   Zheng,   M.   Goddard,   C.  L.   Darlington,   P.   F.   Smith,
Hippocampus  19,  480  (2009).
26.   M.   Goddard,   Y.   Zheng,   C.  L.   Darlington,   P.   F.   Smith,
Behav.   Neurosci.   122,   448  (2008).
27.   R.   W.   Stackman,  A.   S.   Clark,   J.   S.  Taube,   Hippocampus
12,  291  (2002).
28.   S.   Giannetti,   M.   Molinari,  Brain  Res.  Bull.   58,  481
(2002).
29.   D.   M.   Clower,   R.   A.   West,   J.   C.   Lynch,   P.   L.  Strick,
J.   Neurosci.   21,  6283  (2001).
Acknowledgments:   We  thank  C.  De  Zeeuw  for  providing
L7PKCI   mice;  S.   Quet  and  F.   Jarlier  for  technical
supports;   C.  Lamouroux  for  animal   care;   G.  Dallrac
and  K.   Benchenane  for  helpful   comments  on  the
manuscript  and  programming;  and  C.   Lna  for
scientific  insights.   Supported  by  grants  from  Agence
Nationale  de  la  Recherche  (ANR  Young  Researcher
07-JCJC-0108-01  and  ANR-09-EMER-005-02)
(L.R.R.)  and  by  Action  Concerte  Incitative  (ACI)  grant
NIC0027  (B.P.   and  E.S.).
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/385/DC1
Materials  and  Methods
Figs.   S1  to  S5
Tables  S1  to  S3
References
22  April   2011;   accepted  13  September  2011
10.1126/science.1207403
Activity-Dependent  Long-Term
Depression  of  Electrical  Synapses
Julie  S.  Haas,
1,2
*  Baltazar  Zavala,
2
Carole  E.  Landisman
1,2
*
Use-dependent  forms  of  synaptic  plasticity  have  been  extensively  characterized  at  chemical
synapses,  but  a  relationship  between  natural  activity  and  strength  at  electrical  synapses  remains
elusive.  The  thalamic  reticular  nucleus  (TRN),  a  brain  area  rich  in  gap-junctional  (electrical)
synapses,  regulates  cortical  attention  to  the  sensory  surround  and  participates  in  shifts  between
arousal states; plasticity of electrical synapses may be a key mechanism underlying these processes.
We  observed  long-term  depression  resulting  from  coordinated  burst  firing  in  pairs  of  coupled
TRN  neurons.  Changes  in  gap-junctional  communication  were  asymmetrical,  indicating  that
regulation  of  connectivity  depends  on  the  direction  of  use.  Modification  of  electrical  synapses
resulting  from  activity  in  coupled  neurons  is  likely  to  be  a  widespread  and  powerful  mechanism
for  dynamic  reorganization  of  electrically  coupled  neuronal  networks.
T
he thalamic  reticular  nucleus (TRN) is
a shell comprising a homogenous pop-
ulation  of   parvalbumin  (PV)positive  g-
aminobutyric acid(GABA)releasing(GABAergic)
neurons  surrounding  the  dorsal  thalamus  (1,   2).
These cells provide powerful inhibition to thala-
mocortical relay neurons (3) upon integration of
their corticothalamic and thalamocortical  inputs.
In  addition  to  its  proposed  role  in  focusing  the
neural   spotlight   of  attention  (4,   5),   the  TRN  is
strongly  involved  in  regulating  states  of  arousal
(6,   7)  by  means  of  alternation  between  burst
and  tonic  modes  of  firing.   Burst  firing  in  the
TRN  is  a  prominent  component  of  sleep  spin-
dles  (8,   9)  and absence seizures (9,  10), both of
which are marked by dramatic changes in cortical
attention  and  behavioral   responsiveness  to  sen-
sory input.
In   central   mammalian   neurons,   electrical
(gap-junctional)  synapses  appear  all   over  the
brain  (11,   12)   and  mainly  couple   GABAergic
neurons   of   similar   subtype   (1315).   Electrical
synapses contribute to synchrony in coupled net-
works (11, 1621), although computational studies
suggest  that  the  precise  role  of  gap  junctions  in
synchrony can be complex (2224).
Cells in the TRN are densely and powerfully
connected  by  electrical   synapses   (17,   18)   that
persist into adulthood (25) and, as in other areas,
participate  in  its  synchronous  activity  (18).  The
experimentally  isolated  TRN  generates   spindle
rhythms in the absence of other inputs (26), sug-
gesting  that   electrical   synapses  are  likely  to  be
key players in TRN synchrony and in behavioral
switching between firing states.
Activity-dependent   forms  of   plasticity  have
been  extensively  described  at   excitatory  (gluta-
matergic)  chemical   synapses  (27,   28)  and,   to  a
lesser  extent,  at  inhibitory  (GABAergic)  chemi-
cal   synapses   (2931).   Although  the   issue   has
received far less attention than plasticity of chem-
ical synapses, modifications of electrical synapses
have  been  documented  in  a  handful   of   reports
(32, 33). Because electrical synapses are likely to
play  a  major  role  in  coordinating  TRN  activity,
we  sought   to  investigate  the  effects   of   natural
forms of activity in coupled neurons on the strength
of the electrical synapses between them.
We   recorded   from  pairs   of   gap   junction
coupled   TRN  neurons   (Fig.   1A)   within   con-
ventional   thalamocortical   brain  slices  (34).   To
measure electrical synaptic strength, we delivered
hyperpolarizing  current  injections  into  one  neu-
ron (cell 1) while recording voltage (V) responses
in both neurons, which were maintained at a base-
line V
m
 =  65 mV (Fig. 1B). Using these deflec-
tions, we determined the coupling coefficient cc
12
=
DV
cell 2
/DV
cell 1
, and frominjecting current into cell
2, similarly determined cc
21
= DV
cell 1
/DV
cell 2
. We
also calculated  coupling conductance  G
C
 (34)  in
each direction. From a total of 313 paired record-
ings  of  coupled  TRN  neurons,  we  found  an  av-
erage  cc of 0.12  T 0.08 and  G
C
 of 0.80  T 0.63 nS
(mean  T  SD) (Fig. 1C), which is in line with the
values  for  previous  reports  in  TRN  (17,   18,   33)
1
Childrens  Hospital,  Department of  Neurology, Harvard  Uni-
versity,   300  Longwood  Avenue,   Boston,   MA  02115,   USA.
2
Center for Brain Science, Harvard University, 52 Oxford Street,
Cambridge, MA 02138, USA.
*To   whom  correspondence   should   be   addressed.   E-mail:
julie.haas@gmail.com   (J.S.H.);   carole.landisman@hms.
harvard.edu  (C.E.L.)
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   389
REPORTS
and  of   similar   size  to  cc  values  reported  in  the
cortex and other areas (3537). Other parameters,
such as  intraneuronal  distance  and probability  of
coupling, were similar to previous reports (18).
Asymmetry  of   electrical   synapses  has  been
observed  experimentally  (36,   37).   In  our   data,
coupling was rarely symmetrical, which is shown
by the spread of values when plotting  cc
21
 against
cc
12
 for each pair (Fig. 1D). We quantified asym-
metry  by  the  ratio  of  directional   ccs  (cc
21
/cc
12
)
for each pair; for all pairs,  the mean ratio of  ccs
was 1.6  T  0.6 (n = 313 pairs) (Fig. 1E). Some of
Fig.   1.   (A)  Magnification  60  infrared  image  from  patch
recordings  of   a  coupled  pair  of   TRN  neurons.   (B)   Current
injection  into  one  cell (I
1
)  of  a  coupled  pair drives  a  direct
response   in   that   cell   (V
1
)   and   a   gap   junctionrelayed
response in the second cell (V
2
); cc
12
 = DV
2
/DV
1
. Scale bars,
5  mV, 0.1 s. (C)  Mean  electrical synaptic  conductance  (G
C
)
plotted  against   mean  cc   (dots).   Open  circles   are  binned
averages, with a slope of 7.9 [bin width, 0.02; coefficient of
determination (r
2
) = 0.77]. (D) Directional cc (purple, scaled
by   10)   and   G
C
  (orange)   for   each   pair;   12   represents
coupling measured by current injection into cell 1, as in (B).
(E)   Coupling  asymmetry  was  quantified  by  distribution  of
ratios   (cc
12
/cc
21
  and   G
12
/G
21
,   larger   value/smaller;   bin
width, 0.05). (F) Spikes driven by current injection into one
cell   (gray)   caused  spikes  in  the  unstimulated  coupled  cell
(black), as shown for three pairs with cc between 0.2 and 0.4
maintained at baseline V
m
65 mV. Scale bar, 25 mV, 0.1 s.
(G)   Wide-field  image  of   TRN  cells  loaded  with  OGB-Bapta
1AM  (Invitrogen,  Carlsbad,  California).  (H)  Stimulation  of  a
patched  cell   (gray)   drove  bursting  and  strong  calcium  re-
sponses  in  that  cell   and  in  several   neighboring  cells  (scale
bars, 1%  DF/F, 50 ms and 25 mV, 50 ms for bottom trace).
Traces are from the cells labeled by color and number in (G).
I
1
V
2
V
1
0 2 4
0
2
4
12 
2
1
10cc
  G
C
0 0.15 0.3
0
1
2
3
mean cc
m
e
a
n
 
G
C
 
(
n
S
)
1 2 3
0
0.1
0.2
ratio
d
e
n
s
i
t
y
cc
G
C
A B C D E
F
G H
1
2
3
4
5
6
7
8
Fig.   2.   (A)   Paired  bursting  driven  by  simultaneous
current   injections   into  both  cells   of   coupled  pairs.
Scale  bars,  20  mV,  50  ms.  (Inset)  Close-up  of  paired
burst   event.   (B)   Mean  cc  and  G
C
  before  and  after
paired  bursting  (gray  bar).   (C)   Average  normalized
input resistance (R
in
) and membrane potential (V
m
) for
the  neurons  summarized  in  (B).   (D)  Example  paired
responses  before  and  after  activity  pairing  as  in  (A).
Scale  bars,   100  ms,   2.5  mV  (coupled  response,   in
black),   5  mV  (direct  response,   in  gray).   (E)  Bursting
driven by current injections into one cell of a coupled
pair (gray trace) while the other neuron was quiescent
(black trace). Scale bars, 20 mV, 50 ms. (Inset) Close-
up of burst in cell 1 and burstlet in cell 2. (F) Mean cc
and G
C
before and after single-cell bursting (gray bar).
(G)   Average   normalized   input   resistance   (R
in
)   and
membrane potential (V
m
) for the neurons summarized
in (F). (H) Example paired responses before and after
activity pairing as in (E). Scale bars, 100 ms, 2.5 mV
(coupled response, in black), 5 mV (direct response,
in gray).
10 0 10 20
0.8
1
1.2
Elapsed Time (min)
R
i
n
,
 
V
m
 
(
n
o
r
m
)
10 0 10 20
0.8
0.9
1
1.1
G
C
,
 
c
c
 
(
n
o
r
m
)
A
B
C
D
10 0 10 20
0.8
1
1.2
Elapsed Time (min)
R
i
n
,
 
V
m
 
(
n
o
r
m
)
10 0 10 20
0.8
0.9
1
1.1
G
C
,
 
c
c
 
(
n
o
r
m
)
E
F
G
H
control
post
activity
control
post
activity
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 390
REPORTS
the   observed  asymmetry  in   cc   is   due   to  mis-
matches  in  input   resistance;   however,   ratios  of
directionally measured  G
C
 (G
21
/G
12
), which are
independent of input resistance (34), had a mean
of  1.2  T  0.27  (Fig.  1E).
Like  many  thalamic  neurons,   TRN  neurons
spike  in  two  modes:   conventional   fast   sodium-
based tonic spikes and slower low-threshold cal-
cium  spikes  (LTS),   known  as  bursts,   that   are
crowned by a barrage of fast sodium spikes. In
many  pairs  in  the  current  study,  bursts  elicited
by positive current injection into one neuron were
sufficient  to drive bursts in its coupled neighbor
(Fig.   1F).   Imaging  experiments   revealed  that
bursting  activity  driven  in  a  patched  cell  propa-
gated through a network of coupled cells (Fig. 1,
G and H).
To  determine  the  effects  of  bursting  in  cou-
pled  cells   on  electrical   synaptic  strength,   we
tested coupling strength before and after 5 min of
synchronous evoked bursting in pairs of coupled
neurons. Bursting was driven by simultaneous cur-
rent injections of 100 to 300 pAfor 50 ms at 2 Hz
through  the  recording  electrodes  of  both  neu-
rons, which were maintained at membrane poten-
tials   between   65  and   70  mV  by  means   of
steady-state current injection (Fig. 2A). After paired
bursting, cc was reduced by 12.0 T 3.6%, and G
C
was  depressed  by  13.2  T  1.8%  (P  <  0.05,  two-
tailed unpaired  t test,  n = 7 pairs) (Fig. 2B). This
long-term  depression   (LTD)   persisted   for   the
length  of   recordings   (for   at   least   30  min  after
paired  bursting),   with  no  apparent   signs  of   di-
minishing  (Fig.   2B).   There  were  no  significant
changes in input resistance or membrane resting
potential (Fig. 2C), ruling out the possibility that
the observed changes in electrical synaptic strength
reflected changes in the intrinsic properties of the
neurons  at  the  whole-cell  level.   Although  path-
ological   changes  in  internal   calcium  concentra-
tion  are  known  to  affect  gap-junctional  strength
(32, 38), our estimates of the calciuminflux from
the  slow  rate   of   bursting  used  here   are  much
smaller.   Bursting  rates   in  vivo  are  often  faster
than those used here (19,  26).
To determine whether bursting in one neuron
alone is sufficient to induce LTD, we repeated the
activity paradigm, this time only stimulating burst-
ing  in  a  single  neuron  of  a  pair  (Fig.  2E)  while
holding  the  coupled  cell   at   ~70  mV  so  as  to
prevent it frombursting. After single-cell bursting,
cc was reduced by 15.0  T  3.4%, and  G
C
 was re-
duced  by  13.0  T  2.3%  (P  <  0.05,   n  =  11  pairs)
(Fig. 2F). The magnitude of LTD was not signif-
icantly different for the single-cell burst paradigm
fromthe paired-bursting paradigm(unpaired t test).
To   determine   the   contribution   of   sodium
spikes  to  LTD,   we  repeated  the  bursting  para-
digm  in  both  cells  using  a  bath  application  of
1 mM tetrodotoxin (TTX), which completely and
reversibly  blocks  the  quick  barrage  of  sodium-
mediated action potentials crowning the calcium-
mediated  bursts  (Fig.  3A).  After  paired  bursting
in  TTX,   cc  decreased  by  12.3  T  3.2%,   and  G
C
decreased by 11.7  T 2.6% (P < 0.05,  n = 9 pairs)
(Fig.   3B).   We  also  repeated  the  bursting  para-
digm  in  one  cell  alone  in  TTX  (Fig.  3D).  After
single-cell activity in TTX, cc decreased by 6.5  T
2.3%,  and  G
C
  was  reduced  by  6.0  T  2.0%  (P  <
0.05, n = 11 pairs) (Fig. 3E). When depolarized to
rest just below spiking threshold (~40 mV) and
stimulated to spike with 50-ms pulses repeated at
2 Hz, in order to emulate spiking during bursting
without   activating  the  LTS,   coupling  decreased
by a smaller and delayed amount (DG
C
 =  7.2  T
2.0%,  Dcc =  7.0  T 2.8%;  P = 0.03,  n = 8 pairs;
spike frequency during this paradigmwas twice as
slow  as   during  LTS  bursts)   (fig.   S2).   Of   these
activity  paradigms,   the  amount   of   depression
fromsingle-cell bursting in TTXwas significantly
smaller than others [P < 0.05, analysis of variance
(ANOVA)] (Fig. 3H).
Activity  paradigms   in  which  only  one  cell
was  active  allowed  us  to  characterize  the  time
course  of  changes  in  electrical  synaptic  strength
by  measuring  the  amplitude  of  the  postsynaptic
burstlet  in  the  coupled  cell  during  the  5  min  of
Fig.   3.   (A)   Paired  bursting  driven  by  simultaneous
current injections into both cells of coupled pairs, in the
presence of 1 mM TTX. Scale bars, 10 mV, 50 ms. (Inset)
Close-up  of  paired  burst  events.   (B)  Mean  cc  and  G
C
before and after paired bursting in TTX (gray bar). (C)
Average  normalized  input   resistance  (R
in
)   and  mem-
brane potential (V
m
) for the neurons summarized in (B).
(D) Bursting driven by injections of current into one cell
of  a  coupled  pair  (gray  trace)  while  the  other  neuron
was quiescent (black trace), also in TTX. Scale bars, 10
mV, 50 ms. (Inset) Close-up of burst event and burstlet.
(E) Mean cc and G
C
before and after single-cell bursting in
TTX  (gray  bar).  (F)  Average  normalized  input  resistance
(R
in
)   and   membrane   potential   (V
m
)   for   the   neurons
summarized  in  (E).   (G)   Burstlet   amplitudes   (from  Fig.
2E) during single-cell activity plotted against elapsed time
and normalized to final values. (H) Summary of changes
in G
C
for the four paradigms: paired bursting (2B), single-
cell  bursting  (1B),  paired  bursting  in  TTX  (2B  +  T),  and
single-cell   bursting  in  TTX  (1B  +  T).   Asterisk  indicates
significance (P < 0.05, ANOVA).
10 0 10 20
0.8
1
1.2
Elapsed Time (min)
R
i
n
,
 
V
m
 
(
n
o
r
m
)
10 0 10 20
0.8
0.9
1
1.1
G
C
,
 
c
c
 
(
n
o
r
m
)
A
B
C
G
10 0 10 20
0.8
1
1.2
Elapsed Time (min)
R
i
n
,
 
V
m
 
(
n
o
r
m
)
10 0 10 20
0.8
0.9
1
1.1
G
C
,
 
c
c
 
(
n
o
r
m
)
D
E
F
H
0 1 2 3 4
1
1.1
1.2
Elapsed time during pairing (min)
B
u
r
s
t
l
e
t
A
m
p
l
i
t
u
d
e
(
n
o
r
m
)
2B 1B 2B+T 1B+T
20
10
0
 
G
C
 
(
%
)
www.sciencemag.org   SCIENCE   VOL  334   21  OCTOBER  2011   391
REPORTS
activity. For both single-cell bursting and single-
cell bursting in TTX, changes in synaptic strength
(burstlet   amplitude)   reached   their   steady-state
reduced values within 2 min of activity (Fig. 3G).
In two of our activity paradigms, the activity
of the coupled pair, and thus the use of the syn-
apse, was also asymmetrical (Figs. 2E and 3D)
that is, one neuron was active while the other was
quiescent, resulting in largely unidirectional cur-
rent flow across the gap junction channels during
activity. These asymmetrical stimuli allowed us to
investigate  whether  the  LTD  was  also  expressed
asymmetrically. First, we quantified the effects of
activity  on  each  direction  of   coupling,   with  re-
spect  to  the  active  cell.  Coupling  measured  with
current injection into cell 1 (the active cell during
pairing), or outbound coupling, we denote as cc
12
,
whereas coupling measured with current injection
into   the   quiet   cell   2   and   relayed   by   the   gap
junction  back  to  the   active  cell   1,   or   inbound
coupling,   is  cc
21
  (Fig.   4A).   For  full   bursting  in
one neuron (Fig. 4B), the inbound coupling  cc
21
decreased  by  16.0   T   3.4%,   whereas   outbound
coupling, cc
12
, decreased by 8.6 T 3.7%(P < 0.05
for both directions; two-tailed, paired t test, n = 11
pairs) (Fig. 4, C and D). The change in  cc
21
 was
significantly  larger  than  in  cc
12
  (P  <  0.05).   Di-
rectional  conductances  decreased  similarly;   G
21
decreased by 10.8  T 3.2%, and  G
12
 decreased by
6.8  T 3.2% (P < 0.05). For single-cell LTS burst-
ing in TTX (Fig. 4D), inbound coupling,  cc
21
, de-
creased by 10.0  T 3.0% (P < 0.05,  n = 10 pairs),
whereas the change in outbound coupling,  cc
12
,
was not significant (5.5 T 2.7%, P= 0.07, n = 10
pairs)  (Fig.   4G  and  H).   In  TTX,   outbound  G
12
decreased  by  7.5  T  2.0%  (P  =  0.04),   and  G
21
decreased by 6.6  T 2.5% (P = 0.09).
In principle, asymmetrical use of a gap junc-
tion  could  potentially  act  to  either  decrease,   in-
crease, or preserve the pre-activity asymmetry of
coupling in  any given pair.  To examine  the sys-
tematic  effects  of  unidirectional  synapse  use  on
asymmetry,   we  plotted  the  ratios  of   directional
ccs and G
C
s (cc
21
/cc
12
and G
21
/G
12
) for each pair
after   unidirectional   activity  (Fig.   4,   E  and  I,   y
axis) against the initial values (Fig. 4, E and I,  x
axis).   The  identity  line  corresponds  to  coupling
asymmetry that was unaffected by asymmetrical
use  of   the  synapse.   For   full   bursts  in  one  cell,
ratios of ccs increased on average by 9.1  T 2.4%
after activity (P < 0.01,  n = 11 pairs) (Fig. 4E);
this shift represents a systematic trend of greater
change  in  the  coupling  of  inbound  communica-
tion,   cc
21
,   relative  to  outbound  communication,
cc
12
. Ratios of  G
C
 also increased, by 5.0  T 2.2%
(P < 0.05). Changes in asymmetry were not due
to  coordinated  shifts  in  input   resistance;   R
1
/R
2
decreased  by  3.1  T  2.6%  (P  =  0.25).   For   LTS
bursts without sodiumspikes in one cell, ratios of
ccs and  G
C
s fell  along  the  identity  line after ac-
tivity, with an insignificant change in rectification
from initial values (ratio of  ccs: 6.0  T 4.2%,  P =
0.6; ratio of  G
C
s:   0.6  T 2.0%,  P = 0.76; R
1
/R
2
:
5.3  T  3.4%,   P =  0.07;   n  =  10  pairs)  (Fig.  4I),
indicating  that  the  changes  in  rectification  may
be due to sodium spikes. As expected, ratios of
coupling  coefficients  also  did  not   change  sig-
nificantly  for  symmetrical  synaptic  use  (paired
bursting).
Although   activity-dependent   changes   have
been  extensively  described  and  characterized  at
chemical synapses, long-term modification of
electrical synapses by precise patterns of activity
of coupled cells themselves has not yet been de-
scribed. The changes we measured, ~15%, are
small as compared with some changes measured
at chemical synapses. Neurons receive thousands
of individual chemical synaptic inputs, which are
each very small, often distant from the soma, and
of short, stereotyped time courses. Chemical syn-
aptic inputs are orders of magnitude smaller than
are   electrical   synaptic   inputs   and  typically  in-
effective as single voices in driving a cell to spike.
The average coupling measured here (cc = 0.12)
Fig.   4.   (A)   For   activity  in  cell   1,   cc
12
  (blue)   represents   the   outbound
coupling  measured  with  current  injection  into  cell  1,  and  cc
21
  (green)  rep-
resents   inbound  coupling.   (B)   Single-cell   bursting  in  cell   1  (gray)   with
postsynaptic burstlets in cell 2. Scale bars, 15 mV, 25 ms. (C) Inbound cc
21
before and after full bursts in cell 1. (D) Outbound cc
12
 before and after full
bursts in cell 1. (E) Ratios of directional cc [black solid circles; division of the
changes  in  (C)  divided  by  the  changes  in  (D)  for  each  pair]  and  G
C
  (open
circles, P < 0.05 for both cc and G
C
) after full bursts in cell 1, plotted against
initial values. (F) Bursts in cell 1 (gray) in 1 mM TTX. Scale bars, 10 mV, 25 ms.
(G) Inbound cc
21
 before and after bursts in cell 1 in TTX. (H) Outbound cc
12
before and after bursts in cell 1 in TTX. (I) Ratios of directional cc (red solid
squares; P = 0.6) and G
C
 (open squares; P = 0.76) after bursts in cell 1 in TTX,
plotted  against  initial values. ( J)  Model  of  an  asymmetrical gap  junction  as
two  parallel   branches.   R
C
  represents  the  minimum  conductance  (maximum
resistance)   common  to  both  sides  of   the  gap  junction,   and  R
D
  represents
additional, asymmetrical conductance in one direction.
21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencemag.org 392
REPORTS
applied to an average presynaptic burst (~50 mV)
yields a ~6-mV burstlet in a coupled cell, which
persists  for  the  entire  ~50  ms  of  the  burst  (Figs.
1F,  2E,  and  3D);  a  single  burstlet  is  often  large
enough to drive bursts directly in a coupled neigh-
bor (Fig. 1). Areduction by <15%is considerable
for these already strong synapses and is sufficient
to prevent a cells burstlet from driving its neigh-
bor to burst (fig. S1).
By preferentially diminishing coupling inbound
to  bursting  cells,   activity-dependent   LTD  could
unplug single bursting cells froman overly active
or   synchronous   neighbor   or   network  or   adjust
input   preference   between   intra-TRN  electrical
input and input from corticothalamic or thalamo-
cortical  fibers.  The  effects  of  activity-dependent
changes  may  be  more  complex  in  vivo  because
of   multiple  electrical   synapses  and/or   recurrent
synapses between neurons.
What cellular processes might underlie the ob-
served LTDof electrical synapses? Gap junctions
are  plaques  comprising  hundreds  to  thousands
of individual channels. Insertion and deletion of
gap junction  channels is a normal component of
cellular function and a candidate mechanism for
changing  synaptic  strength.   In  addition,   con-
nexin36  (Cx36)   proteins  have  multiple  phos-
phorylation sites (39, 40). Phosphorylation-related
changes  in  coupling  mediated  by  either   protein
kinase A(41, 42) or CamKII (40) as well as  hemi-
channel  conductance  changes  at  Cx35  channels
(43) have been described.
Our  experiments  indicate  that  electrical  syn-
aptic  strength  is  asymmetrical  at  baseline  and  is
further adjustable in a use-directional manner. Re-
sults  in  mice  in  which  Cx36  has  been  knocked
out   indicate   that   synapses   composed   of   non-
Cx36 proteins are more asymmetrical than those
in  wild-type  (44);  thus,  one  possible  source  of
asymmetry   is   inclusion   of   non-Cx36   proteins
and/or  pores  at   the  synapse.   Our  results  further
indicate  that  coupling  asymmetry can  be shifted
by  activity;   neurons   can  fine-tune   the   relative
proportion  of  signals  they  send  or  receive  to  or
from  coupled  neighbors,  respectively.  Increased
expression  or   activation  of   non-Cx36  proteins
could account for this increase in asymmetry.
Despite  evidence  of  gap-junctional  rectifica-
tion  in  mammalian  systems,  the  canonical  sym-
bol for those electrical synapses has remained the
simple  linear  resistor  (R
C
).   Our  observations  of
baseline asymmetry and activity-dependent shifts
in  asymmetry  (Fig.  4E)  led  us  to  reconsider  the
standard  model  because  a  linear  resistor  cannot
account   for   asymmetry  or   increases   in  asym-
metry.  Diodes  have  been  used  to  model  heavily
rectifying invertebrate gap junctions (45) but have
not   yet   been  considered  for   mammalian  gap-
junctional   synapses.   We  suggest   a  model   of   a
mammalian gap-junctional synapse as two branches
in parallel (Fig. 4J): One branch carries the com-
mon  resistance  (R
C
)  or  the  maximum  resistance
(minimum  of   conductance  G
C
)   measured  from
both  directions.   A  parallel   branch  consists  of  a
resistor (R
D
) in series with a diode, representing
the   increase   in   conductance   (or   decreased   re-
sistance) observed as asymmetry.
References  and  Notes
1.   C.   R.   Houser,   J.   E.   Vaughn,   R.   P.   Barber,  E.   Roberts,
Brain  Res.   200,  341  (1980).
2.   P. T. Ohara, A. R. Lieberman, J. Neurocytol. 14, 365 (1985).
3.   D.   Pinault,   M.   Deschnes,   J.  Comp.   Neurol.   391,  180
(1998).
4.   F.   Crick,   Proc.   Natl.   Acad.   Sci.  U.S.A.   81,  4586  (1984).
5.   K.  McAlonan,  J.  Cavanaugh,  R.  H.  Wurtz,  J.  Neurosci.  26,
4444  (2006).
6.   D.   L.   Rowe  et   al.,   Int.   J.   Neurosci.   115,   1273  (2005).
7.   M.   Steriade,   D.   A.   McCormick,  T.   J.   Sejnowski,   Science
262,  679  (1993).
8.   M.   Deschnes,   M.   Paradis,  J.   P.   Roy,   M.   Steriade,
J.   Neurophysiol.  51,  1196  (1984).
9.   M.   Steriade,   Trends  Neurosci.   28,   317  (2005).
10.   M.   Inoue,   J.   Duysens,   J.   M.   Vossen,   A.   M.   Coenen,
Brain  Res.   612,   35  (1993).
11.   M.   V.   Bennett,   R.   S.  Zukin,   Neuron  41,  495  (2004).
12.   B.   W.   Connors,   M.   A.   Long,   Annu.   Rev.   Neurosci.   27,
393  (2004).
13.   M.   Galarreta,   S.   Hestrin,   Nat.  Rev.   Neurosci.   2,  425
(2001).
14.   J.   R.   Gibson,   M.  Beierlein,   B.   W.   Connors,   Nature  402,
75  (1999).
15.   Z.   Chu,   M.   Galarreta,   S.  Hestrin,   J.  Neurosci.   23,  96
(2003).
16.   M.  Beierlein,  J.  R.  Gibson,  B.  W.  Connors,   Nat.   Neurosci.
3,  904  (2000).
17.   C.   E.   Landisman  et  al.,   J.   Neurosci.  22,   1002  (2002).
18.   M.  A.  Long,  C.  E.  Landisman,  B.  W.  Connors,  J.  Neurosci.
24,   341  (2004).
19.   P.   Fuentealba,   M.   Steriade,   Prog.   Neurobiol.   75,   125
(2005).
20.   M.   Blatow  et  al.,   Neuron  38,  805  (2003).
21.   G.   Tams,   E.  H.   Buhl,   A.   Lrincz,   P.   Somogyi,
Nat.   Neurosci.   3,   366  (2000).
22.   K.   Vervaeke  et  al.,   Neuron  67,  435  (2010).
23.   C.   C.   Chow,   N.   Kopell,   Neural   Comput.   12,   1643
(2000).
24.   T.   J.   Lewis,   J.   Rinzel,   J.  Comput.   Neurosci.   14,   283
(2003).
25.   K.   L.   Blethyn,   S.   W.   Hughes,   V.   Crunelli,
Thalamus  Relat.   Syst.   4,  13  (2008).
26.   M.   Steriade,   L.   Domich,   G.   Oakson,   M.  Deschnes,
J.   Neurophysiol.  57,  260  (1987).
27.   R.   C.   Malenka,   M.   F.   Bear,   Neuron  44,   5  (2004).
28.   R.  C.  Froemke,  D.  Debanne,  G.-Q.  Bi,  Front.  Syn.  Neurosci.
2,  19  (2010).
29.   K.   P.   Lamsa,   D.  M.   Kullmann,  M.   A.   Woodin,
Front.   Syn.   Neurosci.   2,  8  (2010).
30.   F. S. Nugent,  J. A. Kauer, J.  Physiol. 586, 1487 (2008).
31.   J.  S.  Haas,  T.  Nowotny,  H.  D.  Abarbanel,  J.  Neurophysiol.
96,  3305  (2006).
32.   A.   E.   Pereda,   D.   S.   Faber,   J.   Neurosci.  16,   983  (1996).
33.   C.   E.  Landisman,   B.  W.   Connors,  Science  310,   1809
(2005).
34.   Materials  and  methods  are  available  as  supporting
material   on  Science  Online.
35.   J. R. Gibson, M. Beierlein, B. W. Connors, J. Neurophysiol.
93,  467  (2005).
36.   A.   Devor,   Y.   Yarom,   J.  Neurophysiol.   87,   3048  (2002).
37.   P.   Mann-Metzer,   Y.   Yarom,   J.   Neurosci.   19,   3298
(1999).
38.   B.   Rrig,   B.  Sutor,   Mol.   Neurobiol.   12,   225  (1996).
39.   W.   W.   Kothmann,   X.   Li,   G.  S.   Burr,   J.   OBrien,
Vis.   Neurosci.   24,  363  (2007).
40.   C.   Alev  et  al.,   Proc.   Natl.   Acad.   Sci.   U.S.A.  105,  20964
(2008).
41.   S.   Urschel   et  al.,   J.   Biol.   Chem.  281,   33163  (2006).
42.   W.   W.   Kothmann,   S.   C.   Massey,   J.   OBrien,   J.   Neurosci.
29,  14903  (2009).
43.   G.   Mitropoulou,   R.   Bruzzone,  J.   Neurosci.   Res.   72,  147
(2003).
44.   T. Zolnik, B. W. Connors, presented at the Society for
Neuroscience Conference, Prog. 42.14. San Diego, CA, 2010.
45.   E.   J.   Furshpan,   D.   D.   Potter,   J.   Physiol.   145,   289
(1959).
Acknowledgments:   We  thank  D.   Feldman  and  K.   Bender
for  valuable  feedback  on  previous  version  of   the
manuscript.   This  work  was  supported  by  the  Milton
Fund.
Supporting  Online  Material
www.sciencemag.org/cgi/content/full/334/6054/389/DC1
Materials  and  Methods
Figs.   S1  and  S2
26  April   2011;   accepted  16  August  2011
10.1126/science.1207502
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POSITIONS   OPEN
TENURE  TRACK  FACULTY  POSITIONS  in
Structural Biology and Dynamics with a focus on
Membrane  Proteins
The  Departments  of  Biochemistry  &  Molecular  Bi-
ology   (website:   http://www.bmb.msu.edu)   and
Chemistry  (website:   http://www.chemistry.msu.
edu)  at  Michigan  State  University  (MSU)  seek  out-
standing  candidates   for   two  tenure-track  ASSIST-
ANT PROFESSORSHIPS in the fields of structural
biology   and  dynamics   with  an  emphasis   on  mem-
brane   proteins   and  biomembranes.   Successful   candi-
dates will develop a vigorous, externally funded research
program  using  and/or  developing  modern  molecu-
lar   biophysical   approaches   to  examine  the  structure
and  dynamics  of   membrane  proteins  involved  in  im-
portant  biological  functions  including  but  not  limited
to,  host  pathogen  interactions,  signaling,   ion  or  mo-
lecular  transport,   bioenergetics,   and  membrane  bio-
genesis. These individuals will have the opportunity to
use state-of-the-art facilities, which include a 900 MHz
NMR,   mass  spectrometry  facility,   and  dedicated  syn-
chrotron  beamlines  at   Argonne  National   Laboratory.
There  are  also  opportunities  to  interact  with  a  diverse
group  of   MSU  faculty  working  in  structural   biology
and dynamics. In addition, the candidates will contrib-
ute  to  teaching  undergraduate,  graduate, and/or med-
ical students  in  their  home department.
Review  of   application  materials   will   begin  on
November  15,   2011  and  will   continue  until   suitable
candidates   are  identified.   The   Departments   are   highly
committed  to  a  diverse  faculty  and  encourage  applica-
tions   from  individuals   in   groups   that   have   been
traditionally   underrepresented   in  science   faculties   in-
cluding  women,   persons   of   color,   veterans,   and  persons
with  disabilities.  Application  materials  should  include
a  single file containing a cover letter, curriculum vitae,
statement   of   research  interests   and  future  directions,
and  the  names   and  e-mail   addresses   of   three  refer-
ences.   All   application  materials  should  be  uploaded
electronically   at   website:   http://www.jobs.msu.
edu  for  Position  #5297.   Questions  regarding  this
position may be directed to Dr. Shelagh Ferguson-
Miller   (e-mail:   fergus20@msu.edu)   in   Biochem-
istry  &  Molecular  Biology  and/or  Dr.  David  Weliky
(e-mail:  weliky@chemistry.msu.edu)  in  Chemistry.
ASSISTANT  OR  ASSOCIATE  PROFESSOR
UCSD  Department  of  Neurosciences
Website:  http://neurosciences.ucsd.edu/
Faculty   Position  for   Neuroscientist   who  studies
genomic  or  epigenomic  control  of  basic  neural  pro-
cesses,   and/or   the  influence  of   genomic   variation
on disease mechanism or therapy. Candidate should
be  familiar   with  neuroscience,   and  have  significant
expertise  with  bioinformatics  tools,   including  high-
resolution  analyses  of   genomic  variation  and  expres-
sion.  Ability  to  integrate  information  across  platforms
is  highly  desirable,   together   with  willingness   to  in-
teract in a highly collaborative environment while pur-
suing independent research interests. Background  in
bioinformatics is  desirable.  Assistant  or  Associate  lev-
el. The La Jolla neuroscience community is extremely
strong  and  diverse,  providing  an  outstanding  oppor-
tunity  to  develop  an  independent  research  program.
Position will be within newly established Translational
Neuroscience  Institute  in the  School  of  Medicine.
Competitive salary and startup. Commensurate with
qualifications and based on University of California pay
scales. Review of applications will begin November 30,
2011  and  continue until the position  is  filled.
Application materials should be submitted via UCSD
AP On-Line RECRUIT (website: https://apol-recruit.
ucsd.edu/),   an  electronic  job  application  system.   See
Position  Posting  10-165  in  RECRUIT.   Please   be
prepared  to  provide   curriculum  vitae,   a   two-page
statement  of  research  interests,   and  three  letters  of
recommendation.
University  of  California, San Diego  is an Affirmative Action/
Equal   Opportunity   Employer   with   a   strong   institutional   com-
mitment  to  excellence  through  diversity.
POSITIONS   OPEN
FACULTY  POSITION
Yale  University  School  of  Medicine
Department  of  Neurobiology
New  Haven,  CT  06520-8001
Website:  http://medicine.yale.edu/
neurobiology/index.aspx
The   Department   of   Neurobiology   at   Yale
University School of Medicine is seeking to hire
a  scientist   using  genetic,   molecular,   or   cellular
approaches to examine nervous system develop-
ment  and  function.  Although  the  emphasis  will
be placed on recruiting an ASSISTANT PRO-
FESSOR,   extraordinary  applicants   at   the  AS-
SOCIATE  PROFESSOR  or   PROFESSOR
levels  will   also  be  considered.   We  seek  excep-
tional candidates with a track record of creativ-
ity  and  productivity, demonstrated potential for
outstanding  future  achievements,  and  a  desire
to participate in a dynamic and growing Neuro-
science community  at Yale. Candidates  are  ex-
pected  to  mount  a  productive  and  innovative
research program, to obtain outside funding, and
to  participate  actively  in  graduate  and  medical
education.
Candidates must hold a Ph.D., M.D., or equiv-
alent   degree.   Please  send  curriculum  vitae,   se-
lected reprints, a research plan, and the names of
at  least  three  references.   All   application  mate-
rials should be sent electronically to the following
e-mail:   neuro.search@yale.edu.   Applications
will   be  reviewed  as  they  are  received,   but  must
be received  before December  1,  2011.
Yale  University  is   an  Affirmative  Action/Equal   Op-
portunity  Employer.   Yale   values   diversity  in  its   faculty,
students,   and   staff   and   especially   welcomes   applications
from  women  and  underrepresented  minorities.
The   Department   of   Biology   at   the   University   of
Minnesota   Duluth  (UMD)   invites   applications   for   a
tenure-track ASSISTANT  PROFESSOR position  in
Genetics,   broadly   defined,   beginning   August   2012.
We seek a person with research experience in genetics,
or   closely  related  field,   who  will   instruct   lecture  and
laboratory courses in genetics, and develop at least one
advanced  course  in  their  area  of   specialization.   The
area  of   specialization  is   open;   applications   from  can-
didates   with   expertise   ranging   from  population  ge-
netics  to  genomics  will   be  equally  considered.   The
successful  candidate  will  establish  an  independent,  ex-
ternally funded research program involving undergrad-
uates,   and  M.S.   and  Ph.D.   students.   Service   to  the
department,   college,   and  University  is   also  expected.
Opportunities  exist  for  collaboration  with  researchers
at UMD_s Natural Resources Research Institute, Large
Lakes  Observatory,   College  of  Pharmacy,   School   of
Medicine,   and  the  EPA  Mid-Continent   Ecology  Di-
vision.   State-of-the-art   research  and  instruction  facil-
ities   and  competitive  startup  funding  are  available.
Essential qualifications include a Ph.D. or terminal de-
gree  in  the  biological  sciences,  evidence  of  potential
for achievement in teaching appropriate for appoint-
ment  at  the  Assistant  Professor  level,   peer-reviewed
publications,  and  strong  oral  and  written  communi-
cation  skills.   The  University  of   Minnesota  requires
that  you  apply  online  for  this  position.   For  a  com-
plete  position  description  and  information  on  how
to apply online, visit website: http://employment.
umn.edu/, and search for Job Requisition 174713.
Complete   applications   will   be   reviewed   beginning
November  22,   2011  and  continue  until   the  position
is filled.  The  University  of  Minnesota  is  an  Equal  Opportunity
Educator  and  Employer.
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21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencecareers.org 396
www.sciencecareers.org   397
UPCOMING FEATURES
Neuroscience: Emerging FieldsNovember 4
Focus on ChinaDecember 9
BS/MS Scientists (online only)January 13
T
his summer, the European Commission announced 
a 7 billion (US$9.6 billion) investment in science, 
its largest funding package ever for research. This 
boost  in  science  capital,  up  9  percent  from  last 
year, is part of the European Unions (EU) Seventh 
Framework Programme for research and technology develop-
ment (FP7), and will fund research that will tackle the biggest 
societal challenges facing Europe and the world. It is expect-
ed to create approximately 174,000 jobs in the short-term and 
450,000  jobs  total,  and  nearly  80  billion  (US$113  billion)  in 
gross domestic product (GDP) growth over 15 years.
This is good news for scientists looking for work in Europe. 
An  integral  part  of  excellence  is  integration  or  mobility  of 
researchers  from  many  different  nations,  says  Michael 
Jennings,  spokesperson  for  Mire  Geoghegan-Quinn, 
European Commissioner of Research, Innovation and Science. 
We  are  investing  in  research  and  innovation  in  Europe  and 
creating  the  conditions  and  priorities  to  better  attract  and 
retain scientists. 
For academics who desire employment on this diverse and 
captivating  continent,  it  is  important  to  remember  that  while 
many  aspects  of  European  science  are  the  same  no  matter 
which  country  you  are  in  (for  example,  all  EU  scholars  can 
apply  for  funds  from  the  European  Research  Council  [ERC]), 
there  are  also  numerous  differences  that  exist  between 
the  members  states  and  their  higher  education  systems. 
The  postdoc  appointment  is  one  such  illustration:  Although 
the  concept  of  postdoctoral  researchers  is  well  understood, 
there is considerable variability in job titles and in the practical 
organization  of  this  stage  in  Europe,  according  to  the  2010 
European Science Foundation (ESF) Report, Research Careers 
in  Europe:  Landscape  and  Horizons  (http://scim.ag/qrFZHZ). 
But  one  thing  is  consistent  across  borders:  Opportunities  for 
employment abound, as long as you know how to navigate the 
member states systems.
GERMANY: STRONG AND OPEN FOR BUSINESS
Germany, with a population of approximately 82 million, seems 
to be faring better than many of its EU neighbors  continued 
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FOCUS ON CAREERS
FOCUS ON EUROPE
 Produced by the Science/AAAS Custom Publishing Office
You  need  to  have  something  to  offersuch  as 
collaborations,  expertise  on  topics  which  would 
complement  theirs,  or  teaching  experiencein 
order to be selected for a permanent position.
                                                     Jani Kotakoski
Academic Opportunities in 
European Science
Norwegian University of 
Science and Technology
Bjrg Elisabeth Kilavik Ryan F. Seipke
Scientists who wish to pursue academic careers in Europe have much with 
which to contend, especially now amidst an uncertain scal landscape. With 
much of the continent still at risk for a recession, there is legitimate reason 
to  be  anxious  over  the  future  of  science  funding  in  the  European  Union. 
However, buttressed by the European Commission, several member states, 
including Germany, the United Kingdom, and France, as well as Scandinavia, 
have plans in place to bolster scientic research and innovation, and make 
those  regions  attractive  destinations  for  early  and  mid-career  professionals 
looking for academic positions. By Alaina G. Levine
Jani Kotakoski
www.sciencecareers.org 398
during this economic tumult. According to the Economist, it is 
in a comfortable scal situation, aided by a strongly growing 
economy  will  help  to  reduce  the  decit  without  tough  public 
spending cuts or tax rises. Cathleen Fisher, president of the 
American Friends of the Alexander Von Humboldt Foundation, 
which promotes and supports the activities of the parent Hum-
boldt Foundation, which provides exchanges between German 
and American scientists, echoes this sentiment. Germany is 
in a relatively good position, having weathered the 2008 nan-
cial crisis quite well, she states.
The nation is advancing in the midst of nancial fragility for 
a variety of reasons, says Andreas Pinkwart, former minister 
for research in North-Rhine-Westphalia, and currently dean of 
HHLLeipzig Graduate School of Management. The German 
economy  has  learned  to  be  very  export-oriented  and  global-
oriented. For example, in the last ve years, the government 
developed  a  ranking  system  for  its  universities  in  an  effort  to 
make them more internationally competitive, he adds. 
This impetus to improve the higher learning institutes is one 
slice of a pie composed of three federal initiatives, which will 
support research and development, student funding, and uni-
versity infrastructure. Each enterprise has its own time frame 
and  budget,  although  the  total  amount  exceeds  20.7  billion 
(US$28.4 billion), and guarantees annual budget increases of 
at least 5 percent for the largest science funding and science 
performance  organizations,  explains  Max Vgler,  director  of 
the North America Ofce of the German Research Foundation 
(DFG, Deutsche Forschungsgemeinschaft). 
Jani Kotakoski, currently an adjunct professor of physics at 
the University of Helsinki, completed his postdoc at Technische 
Universitt Darmstadt. His three-year contract was funded by 
DFG and focused on materials science and high-pressure phys-
ics. I was interested in a permanent position in Germany, he 
says, but I was extremely unlikely to obtain one with the expe-
rience I had at the time. By that point, Kotakoski explains, he 
had completed only one postdoc, which is not usually enough 
experience to be considered a top candidateat least in a eld 
like materials science where the competition is very tough.
He returned to his native Finland and rejoined the group from 
which he had received his Doctorate. Now Kotakoski is on his 
way  to  a  new  position  at  the  University  of Vienna, which  is 
likely  to  greatly  improve  my  research  prole,  he  says.  My 
view is that after two to three years there, I will be able to get 
a  good  position  elsewhere,  like Austria,  Germany,  Finland,  or 
maybe other Nordic countries.
For scientists interested in relocating here, Kotakoski advises 
interested parties to obtain contacts in advance and pursue a 
contract position. One thing to also keep in mind is that the 
people  who  make  the  decision  are  the  other  faculty  mem-
bers, he afrms. Hence, you need to have something to of-
fersuch  as  collaborations,  expertise  on  topics  which  would 
complement theirs, or teaching experiencein order to be se-
lected for a permanent position.
With  a  known  deciency  in  tenure-track  positions,  and  a 
distinctive  tradition  of  requiring  academics  to  complete  a 
second  thesis  (called  Habilitation)  to  even  qualify  for  tenured 
employment, Germany has tried to introduce new paths to-
ward landing these treasured jobs, says Fisher. The addition 
of  junior  professorships  as  an  alternative  to  the  fulllment  of 
a  Habilitation  is  one  such  route,  depending  on  the  institution 
and eld.
Furthermore, it is signicant to note that in Germany, the Ph.D. 
is considered to be an acceptable entry point for industrial jobs. 
Vgler  cites  that  with  2.4  percent  of  the  German  workforce 
holding  Doctorates,  compared  to  an  estimated  1.4  percent  in 
the United States, there is no general expectation to go into 
academia,  he  says.  Pinkwart  comments  that  approximately 
half the Doctorates go to work in industry versus academia.
UK: GETTING BETTER ALL THE TIME
The  United  Kingdom  is  the  third  largest  economy  in  Europe, 
after Germany and France, and is a scientic powerhouse that 
cannot be doubted: With just 1 percent of the worlds popula-
tion, the UK receives over 12 percent of citations to published 
papers, and receives 10 percent of internationally recognized 
prizes each year, according to its embassys website.
But  only  a  decade  ago,  the  government  commissioned 
a  study  in  which  various  problems  that  negatively  affect  the 
supply  chain  of  scientic  academic  jobs  were  identied.  It 
appears  that  this  is  not  an  attractive  career  path  for  many  of 
the  brightest  Ph.D.  graduates. This  is  both  harming  the  UKs 
research  base  and  causing  recruitment  and  retention  difcul-
ties for universities, according to the report led by Sir Gareth 
Roberts, a Welsh physicist. Among the challenges concerning 
postdoctoral and other contract research staff noted were: Un-
certain career prospects associated with work on a short-term 
contractual  basis,  unsatisfactory  training  in  the  skills  required 
in an academic career, and increasingly uncompetitive salaries. 
Today, the UK system still has its troubles. But things seem 
to  be  getting  better,  and  the  nation  continues  to  attract  sci-
entists  from  abroad  to  its  noted  institutions.  Case  in  point: 
Raymond E. Goldstein, the Schlumberger Professor of Com-
plex  Physical  Systems  in  the  Department  of  Applied  Mathe-
matics and Theoretical Physics at the University of Cambridge. 
An  American  who  arrived  in  the  United  Kingdom 
FOCUS ON CAREERS
FOCUS ON EUROPE
 Produced by the Science/AAAS Custom Publishing Office
continued 
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Andreas Pinkwart
The  Alexander  von  Humboldt  Professorships  are  Germanys  way  of  creating  a  beacon  effect
and energising its research landscape. Every year, the Alexander von Humboldt Foundation is
offering  ten  of  the  worlds  leading  researchers  up  to  fve  million  EUR  each  to  create  new  or
consolidate existing internationally visible research focus areas at German universities.
Shine your light in Germany
Proft from excellent conditions for research
Academics of all disciplines are eligible for an Alexan-
der  von  Humboldt  Professorship,  provided  that  they
are  established  abroad  and  recognised  internation-
ally  as  top-class  researchers.  They  will  be  nominated
by  German  universities     where  appropriate  in  co-
operation  with  non-university   research  institutions.
Each  Alexander  von  Humboldt  Professorship  will   be
sponsored  for  a  period  of  fve  years  on  the  premise
that   the   university   presents   a   convincing   strategy
to  sustain  the  position  once  the  funding  period  has
come to an end. Accordingly, universities are asked to
submit  an  implementation  plan  as  part  of  the  fund-
ing  application.   This   will   allow  new,   long-term  re-
search  groups  to  be  established,  conducting  cutting-
edge (international) research. The German Ministry of
Education and Research is supporting this programme.
Visit www.humboldt-foundation.de/ahp for more
information. Next closing dates for applications:
15  November  2011  and  15  May  2012
Alexander von Humboldt Foundation
Jean-Paul-Str. 12
53173 Bonn
Germany
E-Mail: info@avh.de
www.humboldt-foundation.de
Exzellenz verbindet 
be part of a worldwide network.
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www.sciencecareers.org 400
of  higher  education  and  re-
search,  says  a  French  of-
cial  involved  in  the  manage-
ment of bilateral cooperation 
programs.  Initiatives  include 
the  creation  of  a  new  fund-
ing  agency  in  2005,  the 
National  Research  Agency 
(ANR,  LAgence  nationale  de 
la recherch), a decentraliza-
tion  of  universities  to  give 
them  more  independence, 
and  nancial  incentives  to 
internationalize  laboratories, 
which is part of the govern-
ment  push  to  attract  faculty 
from abroad, he describes. 
 One  element  of  Frances  higher  education  is  seemingly 
matchless  in  the  EU:  prior  to  the  last  ve  years,  academia 
offered  only  tenured  positions  explains  the  French  ofcial. 
Now  we  have  contract  positions  also. This  evolution,  com-
bined  with  the  exibility  granted  to  the  institutions  to  recruit 
and negotiate salaries for their research faculty, has helped the 
nation become more attractive to top scientic talent. But the 
completion  of  an  in-country  contract  position  is  still  the  pre-
ferred route to obtaining a professorship.
Bjrg Elisabeth Kilavik can attest to this manner of hiring. 
After completing a postdoc in Marseille, she will start a perma-
nent job as a principal investigator/research scientist at the Na-
tional Center for Scientic Research (CNRS, Centre National de 
la Recherche Scientique). As an employee of the state, Kilavik 
will be subject to a mandatory retirement age, but she will not 
have teaching responsibilities, although this could change. At 
these types of institutions, we are very privileged, she notes.
Kilavik realizes how attractive France is for academics seek-
ing  tenure.  In  Germany,  where  she  completed  her  Ph.D.,  I 
could  maybe  have  gotten  a  ve  year  contract  as  a  junior  pro-
fessor, but there are few possibilities of getting a tenure-track 
position,  she  says.  In  France,  at  least  the  permanent  posi-
tions exist,which gives stability. More people in Europe are 
realizing[France] is close to the only place where these posi-
tions exist. 
SCANDINAVIA: FAIRING WELL AND GROWING
United by similar cultures and language, the Nordic countries of 
Norway,  Sweden,  and  Denmark  support  internationalism  and 
an ease of movement of scholars from one nation to another. 
Almost all universities are state funded, and grants are gener-
ally  bestowed  by  the  individual  countries  research  councils, 
either directly to a PI or through the PIs institution, depending 
upon  the  country  and  type  of  grant. While  many  other  coun-
tries demonstrate scal distress, Scandinavias economies are 
resilient. Norway has a budgetary surplus, and Sweden is debt-
free. All three countries have annually increased spending on 
research and innovation for the last few years.
We are so fortunate in Scandinavia, we are not 
FOCUS ON CAREERS
FOCUS ON EUROPE
continued 
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21  OCTOBER  2011   VOL  334   SCIENCE   www.sciencecareers.org 418
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