SLIDE 1 GRAVITY AS AN EMERGENT FORCE
Erik Verlinde
University of Amsterdam
ICHEP conference, Paris , 22/07/10
SLIDE 2
Emergence
SLIDE 3
SLIDE 4
Current Paradigm
FUNDAMENTAL FORCES: carried by elementary particles
SLIDE 5
Emergence of Particles and Forces
SLIDE 6 Gravity as an Emergent Force
- At a microscopic scale Nature is described by
many degrees of freedom, most of which are invisible and at first sight irrelevant for the
- bserved macroscopic physics.
- Gravity arises due to the fact that the amount of
phase space volume (“information”) occupied by these microscopic degrees of freedom is influenced by the observable macroscopic variables, like the positions of material objects.
SLIDE 7 Black Hole Horizon
- Black hole thought experiments.
Considera particle gradually lowered in to a black hole. Classically, the energy associated with the particle gets redshifted, and vanishes when the particle is at the horizon. Penrose Christodoulou Bekenstein Hawking
SLIDE 8 Black Hole Entropy => Holographic Principle
S BH k B Ac
3
4Gh
Maximal information associated with a part of space can be encoded in a # of bits equal to the area in Planck units
SLIDE 9 ADS/CFT CORRESPONDENCE
EQUIVALENCE BETWEEN FIELD THEORY ON THE “BOUNDARY” AND GRAVITY IN THE “BULK” ONE SPACE DIMENSION EMERGES CORRESPONDING TO THE “SCALE” OF THE BOUNDARY THEORY. RADIAL EVOLUTION IS LIKE RENORMALIZATION GROUP FLOW.
SLIDE 10
Black Hole In AdS space Bulk description Thermal Heat Bath
T
Delocalized state gets thermalized by heath bath
Boundary description:
Particle gets lowered in to black hole
Hot CFT
SLIDE 11
Entropic force (wikipedia)
An entropic force is a macroscopic force whose properties are determined not by the character of an underlying microscopic force, but by the whole system's statistical tendency to increase its entropy.
SLIDE 12
Heat Bath Entropic Force Polymer
T
F T
xS
S(E, x) kB log (E, x)
SLIDE 13 Black Hole Horizon
dx dr 1 2GM / r
E m 1 2GM / r F dE dx GMm r
2
“stretched horizon” black hole
SLIDE 14 Black Hole Horizon
hole thermodynamics implies
F x TH SBH
TH g 2
S BH 2 m x
SLIDE 15
information is stored on holographic screens moving a particle over one Compton wavelength leads to one more bit of information
S 2 k B
x
m
x h mc
A HEURISTIC DERIVATION OF GRAVITY
S 2 k B mc h x
SLIDE 16 To get a force one needs a temperature. By taking that temperature to be the Unruh temperature
- ne finds Newton’s law of inertia
x
m
F x T S
T
k BT 1 2 ha c
F ma
SLIDE 17 In order to get an entropic force I need a temperature
T F
E Mc
2
1 2 k BT
Mc
2 / # bits
# bits Ac
3
Gh
F x T S
F GMm R
2
SLIDE 18
Holographic screens at equipotential (= equal redshift) surfaces
SLIDE 19 What about General Relativity?
Surface of constant redshift
k BT 1 2 h c
Komar mass => Einstein equation
dn c
3
Gh dA
dA 8 GM
log
a a
a
timelike Killing vector
SLIDE 20 T h 2 k B a c
h 2 k B
xS
mc
F ma
Rindler Horizon
F T
xS
ma
c v Suggestive link with QM: What is this velocity v ?
SLIDE 21 Cosmological Horizon
T h 2 k B a0 c
De Sitter Space
a0 c
2
SLIDE 22 Cosmological Horizon
T h 2 k B a
2
a 0
2
c
SLIDE 23 Cosmological Horizon
T h 2 k B a
2
a 0
2
c
h 2 k B dS dx mc a a
2
a 0
2
SLIDE 24 T h 2 k B dv dx
h 2 k B
xS
mv
v
2
2
Equipotential surface v = escape velocity
SLIDE 25 Born-Oppenheimer & Adiabatic theorem
i t (t) H x(t) (t) H x
n ( x)
E n (x)
n ( x)
Schroedinger eqn with H depending on infinitely slow variable Instantaneous eigenstates Adiabatic Reaction Force
F dE n dx ( x )
J pdq 2 nh
Semiclassically
F dE dJ dJ dx
SLIDE 26 Microscopic Fast Variables
Born-Oppenheimer & Entropic Force
x
Macroscopic Slow Variables
x
E
The system stays in an energy eigenstate
- f the fast variables( adiabatic theorem).
SLIDE 27
Born-Oppenheimer & Entropic Force
Macroscopic Slow Variables
x
E
( E , x) d E H ( , x)
d dx log E ( x ), x
Assuming eigenvalues don’t cross, the energy follows from
SLIDE 28
What lives on the screens?
According to string theory: open strings.
Integrating out the UV open strings produces closed strings in the emerged space.
SLIDE 29 Open closed string duality
(-1)
F
ds s
3/2 exp - s(m i 2 i
x
2)
(-1)
F m i d -2
ds s
(5 -d)/2 exp - s i
x
2
(-1)
F m i d -2
d˜ s dk exp
i
ikx ˜ s k
2
x
Open string one loop diagram Massless pole in dual channel
SLIDE 30 UV/IR correspondence
(-1)
F
ds s
3/2 exp - s(m i 2
1
i
x
2)
(-1)
F m i d -2
d˜ s dk exp
i
ikx ˜ s k
2
(-1)
F
ds s
3/2 exp - s(m i 2
1
i
x
2 )
Open string with UV cut off Closed string / gravity with UV cut off
SLIDE 31 Matrix description of gravity.
tr Ý X I
2 ` tr [ X I , X J ] 2
Ý z
2
(x y )
2 z 2
X x11 .. x1N z1 : :: : : x N 1 .. x NN z N z1
*
.. z N
*
yI
SLIDE 32 Matrix description of gravity.
X x11 .. x1N z1 : :: : : x N 1 .. x NN z N z1
*
.. z N
*
yI T
F
SLIDE 33 Gravity as an Emergent Force
- At a microscopic scale Nature is described by
many degrees of freedom, most of which are invisible and at first sight irrelevant for the
- bserved macroscopic physics.
- Gravity arises due to the fact that the amount of
phase space volume (“information”) occupied by these microscopic degrees of freedom is influenced by the observable macroscopic variables, like the positions of material objects.
SLIDE 34
SLIDE 35 Berry Phase and Crossing Eigenvalues
x
E
H z x iy x iy z v x r r B ˆ x 4 r x
2
Dirac monopool At the locus of coinciding eigenvalues
Non-abelian Berry
A ij
i d j
SLIDE 36
SLIDE 37