The document discusses the nature of space and time in the context of physics, arguing that space is not fundamental, while time might be. It explores different theoretical frameworks, like Hamiltonian mechanics and quantum field theory, emphasizing that interactions occur in Hilbert space rather than traditional spatial dimensions. The closure notes speculate on the emergent nature of space and how investigations into quantum gravity could reshape our understanding of these concepts.
space is notfundamental.
time might be.
Sean Carroll, Caltech
http://preposterousuniverse.com/
2.
“What is andis not fundamental”
is not fundamental.
What features will be important ingredients in
an ultimate (as yet hypothetical) comprehensive
theory of everything.
Theories often have very different-looking but
equivalent descriptions (e.g. soliton/particle
duality). Who is to say what is “fundamental”?
But some things are certainly not fundamental;
e.g. temperature. Theories using them are not
comprehensive. Space is like that.
3.
Classical Mechanics
Start witha set of coordinates .
These obey second-order equations of motion:
Specifying the coordinates alone doesn’t determine
a solution; need to give and .
4.
Coordinates qi andmomenta pj.
Hamiltonian function H(qi, pj).
Hamilton’s equations:
Together we have a = {qi, pj}, defining phase space .
A single point a(t0) in  defines a unique trajectory.
Hamiltonian Mechanics
5.
Phase space isa symplectic manifold.
A symplectic form  is a closed, invertible 2-form.
Trajectories are integral curves of the Hamiltonian
vector field,
a(t)
Xa
6.
The coordinate/momentum distinctionis blurred.
Conventionally:
cotangent bundle T*M
= {qi, pi}
= phase space 
configuration space M,
coordinates qi
symplectic form
 =  dpi  dqi
(automatic)
Every cotangent bundle is a symplectic manifold, but
not every symplectic manifold is a cotangent bundle.
Symplecticity is more “fundamental” than
coordinate/momentum distinction.
7.
Mechanics is invariantunder canonical transformations:
{q, p}  {Q(q,p), P(q,p)}
that leave the form of Hamilton’s equations unchanged.
Example:
Nothing “fundamental” about which are the coordinates,
which are the momenta.
Qi = pi ,
Pj = -qj .
8.
Why don’t welive in momentum space?
Think of interacting harmonic oscillators.
Interactions are local in position, not in momentum.
Better:
position is the thing in which interactions are local.
9.
Quantum mechanics
States arerays in Hilbert space: |.
Evolution is governed by the Schrödinger equation:
Energy eigenbasis:
Dynamics are defined by the eigenvalues {En},
the spectrum of the Hamiltonian.
10.
Where is “space”in the quantum state?
We can define a position operator with eigenstates
in terms of which the state is
But we don’t have to; momentum also works.
These are related by Fourier transform,
11.
Or other bases,e.g. creation/annihilation operators
for a simple harmonic oscillator.
Here,
These operators raise and lower energy eigenstates:
12.
Entanglement
For a genericmultiparticle state |,
The wave function is not a function of space,
but of many copies of space.
Things don’t happen in “space”; they happen
in Hilbert space.
Again, it’s locality of interactions that tempts us
to speak otherwise.
13.
Quantum Field Theory
QFTwould seem to deeply privilege “space”; the
Hamiltonian is an integral over space. But why?
Interactions are local in space:
not in momentum:
14.
Gravity
Consider a compactdimension on a circle.
R
A scalar field  can be decomposed
into Kaluza-Klein modes
with energies
From the higher-dimensional perspective, these
modes comprise a tower of massive states.
Conversely: if every field has such a tower,
that implies an extra dimension.
15.
M-theory’s 11th dimension
Witten1995: there are supersymmetric particle
multiplets in Type IIA string theory with masses
that depend on the coupling  as
Small : states are heavy and decouple.
Large : Kaluza-Klein tower, as if an extra dimension.
Q: How many dimensions are
there in string theory?
A: It depends.
x11
10 dimensional
IIA string theory
11 dimensional
supergravity
16.
T-duality: string theoryon a small circle is
equivalent to string theory on a big circle.
Momentum/winding duality.
Mirror symmetries: IIA string theory on one Calabi-Yau
manifold equals IIB string theory on another one.
These are gauge symmetries; exact equivalence.
No such thing as the “true” compactification.
17.
R
Holography
Maximum entropy insidea region
of space doesn’t go as R3, the
volume, but as R2, the area.
Discovered in the context of
black holes, but believed to be more general.
Significance:
The world is not made of separate degrees of
freedom at each point in space.
Emergent space isn’t just a matter of discreteness.
18.
Maldacena, 1997:
quantum gravity
(stringtheory) on
five-dimensional
anti-de Sitter space
times a five-sphere
is equivalent to a
conformal field theory
without gravity on the
four-dimensional boundary.
“The spacetime one is in” is not unambiguously defined.
10 dimensions
AdS5 x S5
4-dimensional
Minkowski space
AdS/CFT
19.
• QM, states,time, & the Schrödinger equation:
Space somehow recovered from |.
• QM, states, & the Wheeler-de Witt equation:
Space and time recovered from |.
• A generalization of, or replacement for, QM.
What might be fundamental?
20.
Closing ruminations
• Space/coordinatesare picked out by the
specific Hamiltonian of the world, not
by the structure of our theories.
• Investigations of quantum gravity provide
strong evidence that space is emergent,
and in a deeper way than local discreteness.
Degrees of freedom are not local.
• Unwarranted speculation: trying to understand
the early universe will help us understand
the role of space & time.