GRAVITY AS AN EMERGENT FORCE Erik Verlinde University of Amsterdam - - PowerPoint PPT Presentation

gravity as an emergent force
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GRAVITY AS AN EMERGENT FORCE Erik Verlinde University of Amsterdam - - PowerPoint PPT Presentation

ICHEP conference, Paris , 22/07/10 GRAVITY AS AN EMERGENT FORCE Erik Verlinde University of Amsterdam Emergence Current Paradigm FUNDAMENTAL FORCES: carried by elementary particles Emergence of Particles and Forces Gravity as an Emergent


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SLIDE 1

GRAVITY AS AN EMERGENT FORCE

Erik Verlinde

University of Amsterdam

ICHEP conference, Paris , 22/07/10

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SLIDE 2

Emergence

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SLIDE 3
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SLIDE 4

Current Paradigm

FUNDAMENTAL FORCES: carried by elementary particles

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SLIDE 5

Emergence of Particles and Forces

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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.

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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

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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

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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.

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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

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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.

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SLIDE 12

Heat Bath Entropic Force Polymer

T

F T

xS

S(E, x) kB log (E, x)

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SLIDE 13

Black Hole Horizon

  • Thought experiment

dx dr 1 2GM / r

E m 1 2GM / r F dE dx GMm r

2

“stretched horizon” black hole

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SLIDE 14

Black Hole Horizon

  • Consistency with black

hole thermodynamics implies

F x TH SBH

TH g 2

S BH 2 m x

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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

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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

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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

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SLIDE 18

Holographic screens at equipotential (= equal redshift) surfaces

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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

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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 ?

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SLIDE 21

Cosmological Horizon

T h 2 k B a0 c

De Sitter Space

a0 c

2

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SLIDE 22

Cosmological Horizon

T h 2 k B a

2

a 0

2

c

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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

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SLIDE 24

T h 2 k B dv dx

h 2 k B

xS

mv

v

2

2

Equipotential surface v = escape velocity

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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

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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).
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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

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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.

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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

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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

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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

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SLIDE 32

Matrix description of gravity.

X x11 .. x1N z1 : :: : : x N 1 .. x NN z N z1

*

.. z N

*

yI T

F

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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.

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SLIDE 34
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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

  • ne can construct

Non-abelian Berry

A ij

i d j

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SLIDE 36
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SLIDE 37