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Tyson, Neil De Grasse, Ph.D.
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Columbia University, 1992
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300 N. ZeebRd.
Ann Arbor, MI 48106
A S t u d y o f t h e A b u n d a n c e D is t r ib u t io n s
A l o n g t h e M in o r A x is o f t h e G a l a c t ic B u l g e
BY
N e il D e G r a s s e T y s o n , b .a ., m .a ., m .phel.
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DISSERTATION
DOCTOR of PHILOSOPHY
in the Graduate School of Arts and Sciences
COLUMBIA UNIVERSITY
1992
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© 1992
N e il D e G r a s s e T y s o n
I present abundance distribution functions for fields along the minor axis of the
Galactic bulge based on CCD photometric observations toward seven windows of low
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extinction. Abundance distribution functions are the most useful form of data to
constrain models of the star formation and the chemical enrichment of the bulge. By
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using the recently-calibrated Washington photometric filter system, the distribution
function in [Fe/H] is determined for each field, and consequently I derive the
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abundance gradient for the bulge. To supplement these observations I analyzed, from
medium dispersion spectra, line strengths of the 33 known bulge carbon stars. The
radial velocities of these carbons stars and of 39 bulge RR Lyrae variables is also
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presented.
from the halo or the disk, 2) the inner bulge underwent no catastrophic mass-loss from
supernova-driven winds or any other mechanism. These scenarios would produce a
different signature in the abundance distributions.
The carbon stars, however, show a gradient in NaD absorption, even for the
inner bulge, with the strongest absorption near the Galactic center. This effect cannot
during the evolution of the star. The Washington system is calibrated to indicate iron
abundance. It may be that the carbon stars are fossils from the first generation of stars
that are enriched by the high-mass-progenitor Type II supemovae. This first generation
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may contain the memory of a dissipational collapse, which results in a gradient in Na
and a-elements (including O and Ti). After collapse, subsequent generations were well
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mixed with the ejecta of the Fe-producing Type I supemovae. Such a hybrid collapse
scenario may have important implications for models of elliptical galaxies and
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spheroidal systems in general. The idea of an early dissipational collapse finds support
in the velocity dispersion of the bulge RR Lyraes where, at ov = 124 ± 15 km s_1, they
have a higher dispersion than high abundance tracers such as the late M giants and the
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[Fe/H]. This is consistent with the notion that the inner bulge is chemically distinct
from the halo while the transition region is a blending of the two. It may be possible to
use kinematics to disentangle the two populations via a radial velocity survey.
A Study of the Abundance Distributions
Along the Minor Axis o f the Galactic Bulge
TABLE OF CONTENTS
Table of C ontents.............................................................................................. i
List of T ables....................................................................................................... v
List of Figures............................................................................................... vii
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List of C harts........................................................................................................ xi
A cknow ledgem ents............................................................................................... xiii
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D ed ication ...............................................................................................................
1.0 In tro d u ctio n ....................................................................................................
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1.1 O verview ................................................................................................. 2
2.0 Carbon Stars:
A Probe of the Bulge Velocity Field and Abundance Gradient 8
2.1.4.3 P a n e ls....................................................................... 39
2.1.5 D iscu ssio n ................................................................................ 49
2.1.6 S um m ary.................................................................................. 53
3.0 RR Lyrae Stars in Baade’s Window: The Velocity Distribution
of a Population withLow Heavy Element Abundance 55
3.1 In troduction........................................................................................ 56
3.2 O bservations...................................................................................... 57
3.3 R eductions........................................................................................... 57
3.4 Radial V elocities.............................................................................. 59
3.5 D iscussion........................................................................................... 64
4.0 The Washington Photometric System....................................................... 69
4.1 In tro d u ctio n ......................................................................................... 70
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4.2 The System ....................................................................................... 71
5.2 O bservations...................................................................................... 86
5.3 R ed u ctio n ............................................................................................ 87
5.3.1 Conversion to Standard System.......................... 88
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5.7 D is c u s s io n ................................................................................................ 125
6.0 Abundance Distribution in Seven Bulge Windows along the Minor Axis.... 128
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6.7 D is c u s s io n ................................................................................................ 182
7.0 C o d a .....................................................................................................................
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R e fe re n c e s .................................................................................................................... 193
A A p p e n d ic e s....................................................................................................... 206
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A.4 Convolution of Gaussian Errors with the Abundance Distribution
of the Simple Model of Chemical Evolution..................... 318
A.4.1 The Convolution................................................ 318
A.4.2 Test for Normal errors..................................... 321
A. 5 Compendium of Abundance Calibrations for Washington Indices 323
A.6 Data Reduction Sequence............................................................ 335
A.6.1 Reduction Sequence........................................... 335
A.6.2 File Extension.................................................... 339
A .6.3 Command File I / O Syntax................................ 340
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A.7 Discussion of Software for Data Management............................ 343
B iographical Sketch........................................................................................ 349
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List o f Tables
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26 Table 2.5 BULGE CARBON STAR VELOCITY DISPERSIONS
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140 Table 6.3 M e a n F ie l d A b u n d a n c e s
TWO-COLOR DIAGRAMS
340 Table A .6.1 REDUCTION FLOW CHART: COMMAND FILE I/O SEQUENCE
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List of Figures
page sub-caption
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function of galactic latitude, (b) CN line strength as a
function of latitude measured in magnitudes.
29 Figure 2.4. Comparison carbon star spectra along side M giant spectra.
31 Figure 2.5.
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NaD correlates with CN.
32 Figure 2.6. Latitude distribution of the 33 bulge carbon stars.
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47 Figure 2.9. Subset of echelle spectra for two carbon bulge stars that
highlights H a absorption.
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76 Figure 4.3. Separation of dwarfs from giants is obtained with the M - 57
index.
77 Figure 4.4. A test of the consistency between the magnesium index, M -
51, and the [Fe/H] derived from the C - M index.
91 Figure 5.1a. Residuals of Table 5.3a plotted for each color transformation.
93 Figure 5.1b. Residuals of Table 5.3b plotted for each color transformation.
95 Figure 5.1c. Residuals of Table 5.3c plotted for each color transformation.
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107-114 Figure 5.3a-h. Dereddened color-color diagrams for the bulge fields.
116 Figure 5.4. Color-color diagram for the gravity-sensitive M-51 index.
118-124 Figure 5.5a-g.
131 Figure 6.1.
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Dereddened color-magnitude diagram for the bulger fields.
Abundances of 18 K giants in Baade’s Window derived
from medium dispersion spectroscopy (Rich 1988) and the
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Washington photometric system.
133 Figure 6.2. Comparison of [Fe/H] for eleven K giants from Rich’s 1988
list that this study has in common with Geisler & Friel
(1990).
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134 Figure 6.3. Check of the temperature sensitivity of the Washington index
T 1-T2 with the more widely used J-K temperature index.
143 Figure 6.4. Derivation of error in abundance.
169 Figure 65. Three plausible abundance distributions from very different
histories of chemical enrichment.
176 Figure 6.8a. Abundance distribution for two contiguous frames at b = -6°.
177 Figure 6.8b. Abundance distribution for two contiguous frames at b = -6°
overlaid with an error-convolved distribution expected for
the closed box simple model of chemical evolution, with
yield Y = 6 Y Q.
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178 Figure 6.9. Abundance distribution for two contiguous frames at b = -8°.
179 Figure 6.10. Abundance distribution at b —-10*.
180 Figure 6.11.
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Abundance distribution at b = -13*.
181 Figure 6.12. Abundance distribution at b = - 17.3*.
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183 Figure 6.13. Galactic latitude dependence of the mean in the abundance
distributions.
188 Figure 7.1. Comparison of the Blanco (1988) M giant counts with two
other profiles for the bulge’s minor axis.
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328 Figure A S A . Iso-abundance curves in the C-Tj and M-T2 colors for -3.0
£ [Fe/H] < +1.0.
329 Figure A S .5. Iso-abundance curves in the M-Tj and T ;-72 colors for +0.5
£ [Fe/H] < -1.0.
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346 Figure A.7.1. Downhill simplex minimization method (in two dimensions)
as used to interpolate abundances from iso-abundance
contours in the two color plane.
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List o f C harts
page description
288 Figure A2.1a. Finding chart overlay # 1 for field: -2.7* Sagittarius III.
289 Figure A.2.1b. Finding chart overlay # 2 for field: -2.7* Sagittarius III.
290 Figure A.2.1c. Field: b = -2.7* Sagittarius HI, Seeing: ~1.2 arc sec.
Epoch 1950: RA 17h 55m 53.5s Dec -29* 07’ 04"
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291 Figure A.2.2a. Finding chart overlay # 1 for field: b = -4°, Baade’s
Window HI. IE
292 Figure A.2.2b. Finding chart overlay # 2 for field: b = —4°, Baade’s
Window HI.
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293 Figure A.2.2c. Field: b = - 4* Baade’s Window IE, Seeing: -1.6 arc sec.
Epoch 1950: RA 18h 88m 12.2s Dec -30* 04' 48"
Window IV.
295 Figure A.2.3b. Finding chart overlay # 2 for field: b = —4", Baade’s
Window IV.
296 Figure A .23c Field: b = —4* Baade’s Window IV, Seeing: -1.2 arc sec.
Epoch 1950: RA 18h 00m 13.0s Dec -30" 00' 03"
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300 Figure A 2 5 a . Finding chart overlay # 1 for field: b = -6° II.
302 Figure A.2.5c. Field: b = -6° II, Seeing: -1.5 arc sec.
Epoch 1950: RA 18h 07m 07.1s Dec -31’ 41' 53"
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305 Figure A.2.7a. Finding chart overlay for field: b = -8* II.
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ACKNOW LEDGEM ENTS
At various stages of this work I have enjoyed and benefitted from conversations
with Dick McCray, Wil van der Veen, Jim Applegate, Jay Frogel, Don Terndrup,
Kevin Predergast, and Ed Shaya. Chapter 3 benefitted especially from conversations
with George Wallerstein, Verne Smith, and Bob Wing. At assorted other times I have
enjoyed conversations about chemical evolution models with Hong Sheng Zhao, about
galactic structure with David Spergel, and about statistics with Robert Lupton.
Doug Geisler was always there when I needed him when I had questions about
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the Washington photometric system, and Peter Stetson and Eileen Friel helped me to
maximize my effectiveness with DAOPhot. I am also grateful to Mario Mateo for
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providing a version of DoPhot in the later phases of this work. I benefitted from
numerous e-mail exchanges with Abi Saha as he helped reveal to me the mysteries of
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RR Lyrae reductions. I am also grateful for the phase corections that Abi provided
from his ephemeris in advance of publication.
The timely completion of this dissertation would not have been possible without
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the energetic programming assistance of Sonya Umar and Roy Gal — two talented
undergraduates who helped to streamline the data reduction. Roy helped primarily with
the carbon star and RRLyrae reductions of Chapters 2 and 3 while Sonya assisted with
the herculean task of managing the DAOPhot reduction procedure for over 100 CCD
frames of data.
As part of the Barnard STEP program I had two ambitious high school seniors,
Samantha Harry and Rafael Verdejo, who produced the preliminary software required
to make finding chart overlays. Another high school student, Morris Matsa, after
proving he really could learn fortran in two days, produced the final version of the
software that made the finding chart overlays of Appendix 2. Morris also made the
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seven-window-panel that appears in the introduction. I am grateful to all three high
school students for their efforts.
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proceed smoothly and permitted me to transcend the expectations of others. His
encouragement and attention to scientific detail — large and small — helped to broaden
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and fine-tune my research skills.
Part of this work was supprted by a NASA graduate fellowship and grant from
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the New York Chapter of the ARCS Foundation. I gratefully acknowledge their
contribution to my professional growth.
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DEDICATION
To my father, Cyril,
for his guiding principles.
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To my mother, Sunchita,
for sharing her love.
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To my brother, Stephen,
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who gives meaning to “brotherhood.”
To my sister, Lynn,
who keeps my feet on Earth.
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I know that I am mortal by nature, and ephemeral;
but when / trace, at my pleasure, the windings to and fro of the heavenly bodies
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I no longer touch earth with my feet:
I stand in the presence o f Zeus, himself, and take my fill o f ambrosia.
IE Claudius Ptolemy
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C h a p te r 1
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Introduction
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It is important not to worship what is known, but to question it.
J. Bronowski
1.1 OVERVIEW
The Galactic bulge is a remarkable compact zoo of stellar populations. For example,
within 1.5 kpc of the Galactic center you will find RR Lyraes and long period variables
(Period ~ 200 d) that coexist with longer period variables (Period > 300 d; OH/IR stars
inclusive), and there are low luminosity carbon stars that coexist with late M giants.
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These pairings represent late stages of stellar evolution that emerge from very different
progenitor populations. In addition, the critical points and principal sequences of the
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color magnitude diagram (main sequence, turnoff, giant branch, horizontal branch) are
all much broader than can be explained by photometric errors alone. In short, the bulge
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populations contain unending observational and theoretical challenges.
Nearly all optical observations of the bulge are conducted through low
extinction “windows” through the plane of the disk. Some lines of sight suffer from 30
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to 60 magnitudes of visual extinction ( Becklin et al. 1978; Glass et al. 1987). A low
extinction region is therefore noticed easily on the Palomar Sky Survey blue plates as
an area of very high star density relative to its surroundings. There are many such
windows at various Galactic latitudes and longitudes. Seven of these windows, along
or near the minor axis, were selected for the photometry of this study. Figure 1.1
presents a schematic (drawn roughly to scale) of five of the lines of sight. As indicated
by the recent COBE image of the Galaxy, the bulge is depicted as flattened. The
concentric ellipses of Fig. 1.1 represent one, two, and three scale heights in an