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Planckian dissipation Jan Zaanen 1 QuickTime™ and a TIFF (Uncompressed) decompressor are needed to see this picture.

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Planckian dissipation

Jan Zaanen

1

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

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The dissipative world of apes …

QuickTime™ and a decompressor

are needed to see this picture.

QuickTime™ and a decompressor

are needed to see this picture.

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The Gross list: the 14 Big Questions

2004

1. The origin of the universe?2. What is dark matter?

11. What is space-time?

0. The origin of temperature, dissipation and probability?

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QuickTime™ and a decompressor

are needed to see this picture.

Subir Sachdev (Harvard)

Sudip Chakravarty (UCLA)

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Plan

1. The dissipative world of apes ….

2. The high Tc superconductivity saga: the past.

3. Viscosity, dissipation and black holes: the AdS/CFT magic

5. Conclusions

4. The high Tc superconductivity saga: the future is critical.

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The second law ….

Dissipation: useful work has to turn into worthless heat …

dSCl

dt 0

Let’s go quantum:

SvN Tr ln

ij ij

eE i

eE i

i

SvN SCl

it ,H

dSvN

dt 0

Von Neumann

Thermal density matrix:

Unitary time evolution:

The second law is beyond quantum physics !!

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Unitarity versus general covariance

Penrose Susskind ‘t Hooft

See also: Van Wezel, Oosterkamp, JZ, cond-mat/0706.3976

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Quantum dissipation in equilibrium worlds

"(k ,)

1

21 e S

k ,

Fluctuation-dissipation theorem:

Green-Kubo-Matsubara

Thermal quantum field theory = Euclidean path integrals

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Wick rotation: time versus temperature

Two point Euclidean correlators:

Analytically continue to ‘our’

Minkowski time => susceptibilities = observables

,r ,

r (0,0)

t,r i,

r

m

m

Measurement time short compared to : „coherent‟

= unitary dynamics

kBT

Measurement time long compared to : „overdamped‟ =

dissipative dynamics

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QuickTime™ and a decompressor

are needed to see this picture.

Subir Sachdev (Harvard)

Sudip Chakravarty (UCLA)

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1

11

1

1

1

1

1

1

1

1

00

0 01

00

0

0 00

1

1

0

0

1

1

0

Hawking Temperature & Entropy

g = acceleration at horizon

A = area of horizon

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Minkowski versus Euclidean black holes

Gibbons-Hawking

Schwarzschild in real time

horizon

Radial distance

Imaginary time

R

kBTHawking

Schwarzschild in imaginary time

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Planck scales

Phenomenon: gravity, matter warps space-time

Characteristic dimensions: Newton’s constant G,

light velocity c.

Planck’s constant carries dimension energy-seconds:

Einstein comes to an end at the Planck scale

Phenomenon: dissipation, work turns irreversibly into heat, takes a characteristic (relaxation) time

Characteristic dimension: temperature

Given hbar, the shortest possible relaxation time is

‘Planckian dissipation’: requires that the quantum

dynamics is scale invariant (quantum critical)!!!!

G G c 5 1042 sec

kBT

Planck

kBT

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Plan

1. The dissipative world of apes ….

2. The high Tc superconductivity saga: the past.

3. Viscosity, dissipation and black holes: the AdS/CFT magic

5. Conclusions

4. The high Tc superconductivity saga: the future is critical.

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The quantum in the kitchen: Landau’s miracle

Kinetic energy

k=1/wavelength

Electrons are waves

Pauli exclusion principle: every state occupied by one electron

Fermi momenta

Fermi energy

Fermi surface of copper

Unreasonable: electrons strongly interact !!

Landau’s Fermi-liquid: the

highly collective low energy quantum excitations are like electrons that do not interact.

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BCS theory: fermions turning into bosons

Fermi-liquid + attractive interaction

Bardeen

Cooper Schrieffer

Quasiparticles pair and Bose condense: D-wave SC: Dirac spectrum

BCS k uk vkck

ck

vac.

Ground state

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Twenty two years ago …

Mueller Bednorz

Ceramic CuO’s,

likeYBa2Cu3O7

Superconductivity jumps to „high‟

temperatures

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Graveyard of Theories

Schrieffer

Anderson

Mueller

Bednorz

Laughlin

Abrikosov

Leggett

Wilczek

Mott

Ginzburg

De Gennes

Yang

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Phase diagram high Tc superconductors

JZ, Science 315, 1372 (2007)

Mystery quantum critical metal‘Stripy stuff’, spontaneous

currents, phase fluctuations ..

BCS k uk vkck

ck

vac.

The return of normalcy

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Divine resistivity

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Fermion sign problem

Imaginary time path-integral formulation

Boltzmannons or Bosons:

integrand non-negative

probability of equivalent classical

system: (crosslinked) ringpolymers

Fermions:

negative Boltzmann weights

non probablistic: NP-hard

problem (Troyer, Wiese)!!!

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Planck scales

Phenomenon: gravity, matter warps space-time

Characteristic dimensions: Newton’s constant G,

light velocity c.

Planck’s constant carries dimension energy-seconds:

Einstein comes to an end at the Planck scale

Phenomenon: dissipation, work turns irreversibly into heat, takes a characteristic (relaxation) time

Characteristic dimension: temperature

Given hbar, the shortest possible relaxation time is

‘Planckian dissipation’: requires that the quantum

dynamics is scale invariant (quantum critical)!!!!

G G c 5 1042 sec

kBT

Planck

kBT

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Quantum criticality or ‘conformal fields’

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Fractal Cauliflower (romanesco)

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The quantum critical response

1

kBT ??

1

T 2

1

1 i

const.

kBT, const.O(1)Planckian

dissipation:

Sachdev

kBT

Scaling form dynamical susceptibility:

1

T 2(

kBT)

Quantum critical regime

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Dissipation in scale-full quantum systems

Example: dissipation in the Fermi-liquid (electron-electron scattering)

nee

2

m inel.

inel. EF

(kBT )2

EF

kBT

EF /kBTIt takes a time longer by

than the Planck time

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Critical Cuprates are Planckian Dissipators

A= 0.7: the normal state of optimallly doped

cuprates is a Planckian dissipator!

1(,T) 1

4

pr

2 r

1 2 r

2, r A

kBT

van der Marel, JZ, … Nature 2004:Optical conductivity QC cuprates

Frequency less than temperature:

[

kBT1] const.(1 A2[

kBT]2)

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Divine resistivity

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‘Real’ hydrodynamics:

Planckian viscosity

1

Planckian dissipation:

kBT

Viscosity, entropy density:

Planckian viscosity:

p

s p

T

s T

kBT

s

kB

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Plan

1. The dissipative world of apes ….

2. The high Tc superconductivity saga: the past.

3. Viscosity, dissipation and black holes: the AdS/CFT magic

5. Conclusions

4. The high Tc superconductivity saga: the future is critical.

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boundary:

d-dim space-time

Hawking radiationgluons

Black holes

strings

quarks

AdS/CFT correspondence: String theory Magic!

d-dim. gauge theory (d+1)-dim string theory

/ conformal field theory / gravity theory

Maldacena

Witten, Gubser,Klebanov,Polyakov

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s

The bulk: Anti-de Sitter space

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The boundary: conformal fields or quantum

criticality!

GR in Anti de Sitter space

Quantum-critical fields on the boundary

Planckian dissipation!

Black hole temperature entropy

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Quantum critical dynamics: classical waves in AdS

WCFT J SAdS x0

0 J

gYM

2 N R4

gYM

2 gs

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E-field

transverse E-field <=> 3d electric field

radial E-field <=> 3d charge density

B-field

radial B-field <=> 3d magnetic field

transverse B-field <=> 3d current density

spatial metric perturb.

transverse gradient <=> 3d distortion

radial gradient <=> 3d stress tensor

temporal metric perturb.

transverse gradient <=> temperature gradient

radial gradient <=> heat flow

SUSY Einstein-Maxwell in AdS <==> SUSY Yang-Mills CFT

The AdS/CFT dictionary

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Dissipation = absorption of classical waves by Black

hole!

Viscosity: absorption cross section of gravitons by black hole

Entropy density s: Bekenstein-Hawking BH entropy = area of horizon

abs 0 16G

= area of horizon (GR theorems)

Universal viscosity-entropy ratio for CFT‟s with gravitational dual limited in

large N by:

s1

4

kB

Hartnoll-Son-Starinets (2002):

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‘Real’ hydrodynamics:

Planckian viscosity

1

Planckian dissipation:

kBT

Viscosity, entropy density:

Planckian viscosity:

p

s p

T

s T

kBT

s

kB

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4kB

s

AdS/CFT viscosity Kovtun-Son-Starinets (2005)

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The quark-gluon plasma

Relativistic Heavy Ion Collider

Quark-gluon ‘fireball’

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The tiny viscosity of the Quark-Gluon plasma

QG plasma: within 20% of the AdS/CFT viscosity!

4kB

s

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S=1/2 Fermi gas at a Feshbach resonance

Very cold fermionic atoms

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RG fixed point described by a “non-relativistic”

CFT: special gravitational AdS dual

Quantum criticality at the Feshbach resonance

See arXiv:0804.3972,0804.4053,0806.2867,0806.3244,0807.1100,0807.1111

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T. Schafer, Phys. Rev. A 76, 063618 (2007); A. Turlapov et. al., J. Low Temp. Physics 150, 567 (2008)

s1

4

kBQuark Gluon plasma

Ultracold 6-Li gas at Feshbach resonance

Planckian dissipation in the atom trap

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Plan

1. The dissipative world of apes ….

2. The high Tc superconductivity saga: the past.

3. Viscosity, dissipation and black holes: the AdS/CFT magic

5. Conclusions

4. The high Tc superconductivity saga: the future is critical.

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Thermo-electric transport at the insulator-superfluid QPT.

Hartnoll, Kovtun, Müller, Sachdev,

Phys. Rev. B 76 144502 (2007)

E.g. Nernst effect:

AdS: graviton-photon cross correlators in the presence of a dyonic black hole!

Stripy cuprates: Ong group

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Why Tc is high …JZ, Nature 430, 512(2004)

Fermionic quantum critical state

BCS type transition: pairs form at Tc

2 bosone1/

2 3.5kBTc

Need the Fermi energy!

But BCS wisdoms like:

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The hairy black holeHartnoll, Herzog, Horowitz, arXiv:0803.3295

Condensate „atmosphere‟

2 0

kBTc

8

AdS-CFT

BCS-like Superconductor on the boundary!

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

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Scale invariance versus BCS

J.-H. She

Gap equation:

1pp(kBT,,B) 0

Fermi-liquid:

Glue strength

Glue frequencySC gap

pp kBT, lnEF B

kBT,

kBTc Be1/, 2 3.5kBTc

Fermionic qu. critical:

Tc is large for moderate glue, gap to Tc ratio “universal” number!

pp kBT, 1

kBT

d2 pp

z

,1

i

d2 pp

z

kBTc B / 2B

c

2z

z

z

2z

, 2 A kBTc

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Cracking the Fermion signs: AdS-to-ARPES

Classical „Dirac waves‟

In progress ….

Schalm Sadri

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In conclusion …

Planckian dissipation: the beautiful hydrodynamic behaviors of quantum critical states of matter.

With help of string theory: this is in literal, but dual correspondence with the physics of black holes.

This sheds unexpected light on real life physics: the quark-gluon plasma and cold atoms.

AdS/CFT might well be the mathematics behind the enigma called High Tc superconductivity !

Further reading: Nature 430, 512 (2004), Science 315, 1372 (2007), Nature 448, 1000 (2007), Science 319, 1205 (2008); Hartnoll, Science 322, 1639 (2008)

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The dissipative world of apes …

QuickTime™ and a decompressor

are needed to see this picture.

QuickTime™ and a decompressor

are needed to see this picture.

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The fundamental constants

, c,G, e,

, c,G, e, kB

Boltzmann‟s constant is the conversion factor between time and probability !?

?

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In conclusion …

Planckian dissipation: the beautiful hydrodynamic behaviors of quantum critical states of matter.

With help of string theory: this is in literal, but dual correspondence with the physics of black holes.

This sheds unexpected light on real life physics: the quark-gluon plasma and cold atoms.

AdS/CFT might well be the mathematics behind the enigma called High Tc superconductivity !

Further reading: Nature 430, 512 (2004), Science 315, 1372 (2007), Nature 448, 1000 (2007), Science 319, 1205 (2008); Hartnoll, Science 322, 1639 (2008).

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empty

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Empty

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Empty

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Penrosian gravitational wave function collapse

Unitary/entangled/microscopic:

Dissipative/collapsed/macroscopic:

| Live > + | Dead >| Live > or | Dead >

id

dtLive

Live H Live

id

dtDead

Dead H Dead

d

dtLive

d

dtdead

Condition for unitarity: global time like Killing vector

Einstein gravity = „gauge theory of diffeomorphism‟: global time like killing vector does not exist in universes with different mass distributions!

Conflict becomes manifest at „collapse time‟:

coll.

G

L

GM 2

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Measuring quantum gravity

Penrosian collapse: ‘it takes a Schroedinger state made from e-coli’s one micrometer apart one second to collapse.’

Flux qubits closest approach with available technology!

MicroAmp currents, cross section 1 micron, height 0.1 mm:

Collapse time of order of seconds!

Van Wezel, Oosterkamp, JZ (cond-mat/0706.3976, Phil. Mag. B)

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The high Tc enigma

200oC

temperature

Quantum critical fermion matter

Electron correlations

conductor

Strangemetal

Super-

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69

Quantum Phase transitions

Quantum scale invariance emerges naturally at a zero temperature continuous phase transition driven by quantum fluctuations:

JZ, Science 319, 1205 (2008)

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Quantum critical QCD ??

Quantum phase transition ????

Quantum critical hydrodynamics

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71

The quark-gluon plasma

Relativistic Heavy Ion Collider

Quark-gluon ‘fireball’

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72

QuickTime™ and aYUV420 codec decompressor

are needed to see this picture.

boundary:

d-dim. Space-time

Hawking radiationgluons

strings

quarks

Black holes

High Tc superconductivity

Quark-gluon plasma

String theory: „AdS/CFT correspondence‟

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AdS/CFT dictionary:

E-field

D transverse E-field <=> D-1 electric field

D radial E-field <=> D-1 charge density

B-field

D radial B-field <=> D-1 magnetic field

D transverse B-field <=> D-1 current density

spatial metric perturb.

D transverse gradient <=> D-1 distortion

D radial gradient <=> D-1 stress tensor

temporal metric perturb.

D transverse gradient <=> D-1 temperature gradient

D radial gradient <=> D-1 heat flow

SUSY Einstein-Maxwell in AdS <==> SUSY Yang-Mills CFT

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74

Finite temperature fields: Euclidean Path Integrals

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75

Nernst effect: experiment

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AdS/CFT dictionary:

E-field

transverse E-field <=> 3d electric field

radial E-field <=> 3d charge density

B-field

radial B-field <=> 3d magnetic field

transverse B-field <=> 3d current density

spatial metric perturb.

transverse gradient <=> 3d distortion

radial gradient <=> 3d stress tensor

temporal metric perturb.

transverse gradient <=> temperature gradient

radial gradient <=> heat flow

SUSY Einstein-Maxwell in AdS <==> SUSY Yang-Mills CFT

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Nernst effect: outcomes

Experiment Phuan Ong et al.

Qui ckTi me™ and a decompressor

are needed to see this pi cture.

AdS-CFT computation: Hartnoll, Kovtun, Mueller, Sachdev

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Superfluid-Mott insulator Quantum phase transition

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Optical conductivity near 2+1D superfluid-Mott

insulator QPT

g

SF

QC

MI

1()

79

Hartnoll, Herzog,Horowitz, arXiv:0803.3295

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Fermionic quantum phase transitions

JZ, Science 319, 1205 (2008)

„Mystery‟quantum critical metal (fermions !!)

JZ, Nature 430, 512 (2004)

High Tc superconductors

Heavy fermion metals

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Breaking SUSY CFT by chemical potentials …

g

QC

81

and supersymmetric!

Driving away from criticality by imposing finite fermion and boson charge density.Breaks scale invariance …

and supersymmetry!

Like fermion-boson model (?):

H bb f f (b f f f f b)

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Boson and Fermion pair optical conductivity

82

2 0

kBTc

8

Bose field:

Fermion pair field!

BCS like temperature dependence with

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Fermionic quantum criticality??

83

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84

Sachdev

She

Sadri

Schalm

Verlinde

McFadden

me

JZ: ‘A black hole full of answers’, Nature 448, 1001

(2007)

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85

The Viscosity-Entropy ratio Hartnoll-Son-Starinets (2002)

0L

1

2dtd

x e it Txy (t,

x ),Txy (0,0)

0L

q0L ImGxy,xy

R ,q

abs 16G

ImGR

abs 0 16G

s1

4

kB

CFT viscosity, Kubo formula:

AdS correspondent: graviton absorption cross section by black hole:

= area of horizon (GR theorems)

CFT entropy density: AdS correspondent = BH entropy = area of horizon

Universal viscosity-entropy ratio for CFT‟s with

gravitational dual:

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Conformal symmetry = quantum criticality

Supersymmetry <==> non-renormalization theorems „Planes of strongly interacting unstable fixed points‟AdS is the „geometrical dual‟ of conformal

invariance

Black holes, gauge background sources, etcetera, break conformal invariance

AdS/CFT is merely a „generating functional‟ of fanciful scaling

analysis ????

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87

Why do I care?

Roger Penrose Darius Sadri

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88

AdS/CFT for finite temperature hydrodynamics

Finite temperature fields: imaginary time compactification radius

R

kBT

Are there AdS spaces that are periodic in Euclidean time?

Yes, two (Hawking-Page, Witten):

(1)EAdS (low T confined phase, no entropy)

(2) Black hole in AdS (high T deconfined phase, entropy)

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89

‘Nernst regime’: fluctuating

superconducivityFinite temperature hydrodynamics of superconductor-insulator QCP??

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Ceperley path integrals and fermionic quantum

criticalityFermi-Dirac statistics encoded in ‘nodal surface constraints’ : probablistic theory.

Explicit example: Feynmannian Fermionic back flow, fractal nodal surface and quasiparticle effective mass divergence.

Krueger, JZ, arXiv:0804.2161

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The AdS/CFT challenge: fermionic quantum criticality

Heavy Fermion metals

JZ, Science 319, 1205 (2008)

High Tc Superconductors

JZ, Nature 430, 512 (2004)

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1

11

1

1

1

1

1

1

1

1

00

0 01

00

0

0 00

1

1

0

0

1

1

0

Hawking Temperature & Entropy

g = acceleration at horizon

A = area of horizon

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Strings and Black Holes

Universal physics of 0+1D Black hole <=> 1+1D CFT

● A classical = cosmic string is a Black string ● String theory has non-perturbative extended objects (like strings/vortices) called (mem)branes with p spatialdimensions

CLAIM:For certain (extremal) Black p-branes the universal (near horizon) brane physics is described by a p+1 dimensional CFT

[Maldacena]

The near-horizon of an extremal black brane is anAnti-de-Sitter space (homogeneous negative curvature)

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Viscosity/Entropy ratio

- Kubo formula = Zero frequency absorption of graviton by BH

- Zero frequency absorption of a graviton by BH = Area

- BH entropy = Area [Hawking]

Viscosity/Entropy ratio is order (1)!

[ In pQCD long calculation Visc/entropy ~ 1/g2ln(g)

[Arnold, Moore, Yaffe]]

[Policastro, Son, Starinets]

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kB

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Conformal symmetry = quantum criticality

AdS is the ‘geometrical dual’ of conformal invariance● Black holes, gauge sources break conformal invariance●

Supersymmetry <==> non-renormalization theorems●

● ‘Planes of unstable (strongly interacting) quantum critical

points’

AdS-CFT is ‘generating functional’ of fanciful scaling analysis ????

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Thermo-electric response coefficients

Kubo formula, e.g.

Hartnol, Kovtun

Muller, Sachdev

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(d+1)-dim Dyonic AdS Black Hole

metric + B-field fluctuations

linearized Einstein-Maxwell equation =>

two point functions of heat flow and electric currents.

thermo-electric coefficients follow from Kubo formula

dyonic AdS black holes exhibit Nernst effect!Hartnol, Kovtun

Muller, Sachdev

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(d+1)-dim AdS Black Hole = d-dim Thermal CFT

Black hole + metric fluctuations

linearized Einstein equation => quadratic Einstein action

= sufficient to compute two point functions of stress tensor.

Two point functions follow from free wave propagation

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AdS/CFT

Map of theories: map of 5d to 4d correlation functions

[Follows from open-closed string duality]

A Duality[Note: CFT sources are AdS fields] [Maldacena, Witten

Gubser, Klebanov,

Polyakov]

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String Theory for RHIC physics

● meson melting at high J● Mach cones due to heavy quarks

● Photon Production Rates● J/Psi screening● ...

Conceptually very simple calculations compared to (strong coupling) QCD

with answers very close to experiment (5-30%)

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Benefits from a natural point of view

AdS/CFT: ● CFTs are scale invariant

● CFTs: universal dynamics of continuous phase transitions

universal

...String theory for the real world?

universal

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Viscosity:

Kubo formula

Viscosity of the thermal conformal field theory

is computed from scattering of gravity waves off

an AdS black hole background

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Gauge/String Duality