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AdS/CFT correspondence and hydrodynamics. Andrei Starinets. Oxford University. From Gravity to Thermal Gauge Theories: the AdS/CFT correspondence. Fifth Aegean Summer School Island of Milos Greece. September 21-26, 2009. Plan. I. Introduction and motivation. II. Hydrodynamics

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ads cft correspondence and hydrodynamics

AdS/CFT correspondence and hydrodynamics

Andrei Starinets

Oxford University

From Gravity to Thermal Gauge Theories: the AdS/CFT correspondence

Fifth Aegean Summer School

Island of Milos

Greece

September 21-26, 2009

slide2

Plan

I. Introduction and motivation

  • II. Hydrodynamics
  • hydrodynamics as an effective theory
  • linear response
  • transport properties and retarded correlation functions
  • III. AdS/CFT correspondence at finite temperature and density
  • holography beyond equilibrium
  • holographic recipes for non-equilibrium physics
  • the hydrodynamic regime
  • quasinormal spectra
  • some technical issues
slide3

Plan (continued)

  • IV. Some applications
  • transport at strong coupling
  • universality of the viscosity-entropy ratio
  • particle emission rates
  • relation to RHIC and other experiments

Some references:

D.T.Son and A.O.S., “Viscosity, Black Holes, and Quantum Field Theory”, 0704.0240 [hep-th]

P.K.Kovtun and A.O.S., “Quasinormal modes and holography”, hep-th/0506184

G.Policastro, D.T.Son, A.O.S., “From AdS/CFT to hydrodynamics”, hep-th/0205052

G.Policastro, D.T.Son, A.O.S., “From AdS/CFT to hydrodynamics II: Sound waves”, hep-th/0210220

slide5

Over the last several years, holographic (gauge/gravity duality) methods

were used to study strongly coupled gauge theories at finite temperature

and density

These studies were motivated by the heavy-ion collision programs at RHIC

and LHC (ALICE, ATLAS) and the necessity to understand hot and dense

nuclear matter in the regime of intermediate coupling

As a result, we now have a better understanding of thermodynamics

and especially kinetics (transport) of strongly coupled gauge theories

Of course, these calculations are done for theoretical models such as

N=4 SYM and its cousins (including non-conformal theories etc).

We don’t know quantities such as for QCD

slide6

Heavy ion collision experiments at RHIC (2000-current) and LHC (2009-??)

create hot and dense nuclear matter known as the “quark-gluon plasma”

(note: qualitative difference between p-p and Au-Au collisions)

Evolution of the plasma “fireball” is described by relativistic fluid dynamics

(relativistic Navier-Stokes equations)

Need to know

thermodynamics(equation of state)

kinetics(first- and second-order transport coefficients)

in the regime of intermediate coupling strength:

initial conditions(initial energy density profile)

thermalization time(start of hydro evolution)

freeze-out conditions(end of hydro evolution)

slide7

Energy density vs temperature for various gauge theories

Ideal gas

of quarks

and gluons

Ideal gas

of hadrons

Figure: an artistic impression from Myers and Vazquez, 0804.2423 [hep-th]

slide8

Quantum field theories at finite temperature/density

Equilibrium

Near-equilibrium

transport coefficients

emission rates

………

entropy

equation of state

…….

perturbative

non-perturbative

perturbative

non-perturbative

????

Lattice

kinetic theory

pQCD

slide9

II. Hydrodynamics

L.D.Landau and E.M.Lifshitz, Fluid Mechanics, Pergamon Press, Oxford, 1987

D.Forster, Hydrodynamic Fluctuations, Broken Symmetry, and Correlation Functions,

Benjamin/Cummings, New York, 1975

P.K. Kovtun and L.G.Yaffe, “Hydrodynamic fluctuations, long-time tails, and supersymmetry”,

hep-th/0303010.

slide10

The hydrodynamic regime

Hierarchy of times (e.g. in Bogolyubov’s kinetic theory)

0

t

|

|

|

|

Mechanical

description

Hydrodynamic

approximation

Equilibrium

thermodynamics

Kinetic

theory

Hierarchy of scales

(L is a macroscopic size of a system)

slide11

The hydrodynamic regime (continued)

Degrees of freedom

|

|

|

|

0

t

Hydrodynamic

approximation

Equilibrium

thermodynamics

Mechanical

description

Kinetic

theory

Coordinates,

momenta of

individual

particles

Coordinate-

and time-

dependent

distribution functions

Local densities

of conserved charges

Globally conserved

charges

Hydro regime:

slide12

Hydrodynamics: fundamental d.o.f. = densities of conserved charges

Need to add constitutive relations!

Example: charge diffusion

Conservation law

Constitutive relation

[Fick’s law (1855)]

Diffusion equation

Dispersion relation

Expansion parameters:

slide13

Example: momentum diffusion and sound

Thermodynamic equilibrium:

Near-equilibrium:

Eigenmodes of the system of equations

Shear mode (transverse fluctuations of ):

Sound mode:

For CFT we have

and

what is viscosity
What is viscosity?

Friction in Newton’s equation:

Friction in Euler’s equations

viscosity of gases and liquids
Viscosity of gases and liquids

Gases (Maxwell, 1867):

Viscosity of a gas is

  • independent of pressure
  • scales as square of temperature
  • inversely proportional to cross-section

Liquids (Frenkel, 1926):

  • Wis the “activation energy”
  • In practice, A and W are chosen to fit data
slide16

“For the viscosity…expansion was developed by Bogolyubov in 1946 and this remained the standard reference

for many years. Evidently the many people who quoted Bogolyubov expansion had never looked in detail at more

than the first two terms of this expansion. It was then one of the major surprises in theoretical physics when

Dorfman and Cohen showed in 1965 that this expansion did not exist. The point is not that it diverges,

the usual hazard of series expansion, but that its individual terms, beyond a certain order, are infinite.

first order transport kinetic coefficients
First-order transport (kinetic) coefficients

Shear viscosity

Bulk viscosity

Charge diffusion constant

Supercharge diffusion constant

Thermal conductivity

Electrical conductivity

* Expect Einstein relations such as to hold

slide18

Second-order hydrodynamics

Hydrodynamics is an effective theory, valid for sufficiently small momenta

First-order hydro eqs are parabolic. They imply instant propagation of signals.

This is not a conceptual problem since hydrodynamics becomes “acausal” only

outside of its validity range but it is very inconvenient for numerical work on

Navier-Stokes equations where it leads to instabilities [Hiscock & Lindblom, 1985]

These problems are resolved by considering next order in derivative expansion,

i.e. by adding to the hydro constitutive relations all possible second-order terms

compatible with symmetries (e.g. conformal symmetry for conformal plasmas)

second order transport kinetic coefficients
Second-order transport (kinetic) coefficients

(for theories conformal at T=0)

Relaxation time

Second order trasport coefficient

Second order trasport coefficient

Second order trasport coefficient

Second order trasport coefficient

In non-conformal theories such as QCD, the total number of second-order transport

coefficients is quite large

slide20

Derivative expansion in hydrodynamics: first order

Hydrodynamic d.o.f. = densities of conserved charges

or

(4 equations)

(4 d.o.f.)

slide21

First-order conformal hydrodynamics (in d dimensions)

Weyl transformations:

In first-order hydro this implies:

Thus, in the first-order (conformal) hydro:

slide25

Supersymmetric sound mode (“phonino”) in

Hydrodynamic mode

(infinitely slowly relaxing

fluctuation of the charge

density)

Hydro pole

in the retarded

correlator of the

charge density

Conserved

charge

Sound wave pole:

Supersound wave pole:

Lebedev & Smilga, 1988 (see also Kovtun & Yaffe, 2003)

slide28

In quantum field theory, the dispersion relations such as

appear as poles of the retarded correlation functions, e.g.

- in the hydro approximation -

computing transport coefficients from first principles
Computing transport coefficients from “first principles”

Fluctuation-dissipation theory

(Callen, Welton, Green, Kubo)

Kubo formulae allows one to calculate transport

coefficients from microscopic models

In the regime described by a gravity dual

the correlator can be computed using

the gauge theory/gravity duality

spectral function and quasiparticles
Spectral function and quasiparticles

A

B

A: scalar channel

C

B: scalar channel - thermal part

C: sound channel

slide31

III. AdS/CFT correspondence

at finite temperature and density

slide32

4-dim gauge theory – large N,

strong coupling

10-dim gravity

M,J,Q

Holographically dual system

in thermal equilibrium

M, J, Q

T S

Deviations from equilibrium

Gravitational fluctuations

????

and B.C.

Quasinormal spectrum

slide33

Dennis W. Sciama (1926-1999)

P.Candelas & D.Sciama, “Irreversible thermodynamics of black holes”, PRL,38(1977) 1732

slide34

From brane dynamics to AdS/CFT correspondence

Open strings picture:

dynamics of coincident D3 branes

at low energy is described by

Closed strings picture:

dynamics of coincident D3 branes

at low energy is described by

conjectured

exact equivalence

Maldacena (1997); Gubser, Klebanov, Polyakov (1998); Witten (1998)

slide35
Field content:

supersymmetric YM theory

Gliozzi,Scherk,Olive’77

Brink,Schwarz,Scherk’77

  • Action:

(super)conformal field theory = coupling doesn’t run

slide36

AdS/CFT correspondence

conjectured

exact equivalence

Latest test: Janik’08

Generating functional for correlation

functions of gauge-invariant operators

String partition function

In particular

Classical gravity action serves as a generating functional for the gauge theory correlators

slide37

AdS/CFT correspondence: the role of J

For a given operator , identify the source field , e.g.

satisfies linearized supergravity e.o.m. with b.c.

The recipe:

To compute correlators of , one needs to solve the bulk

supergravity e.o.m. for and compute the on-shell action

as a functional of the b.c.

Warning: e.o.m. for different bulk fields may be coupled: need self-consistent solution

Then, taking functional derivatives of gives

slide38

Holography at finite temperature and density

Nonzero expectation values of energy and charge density translate into

nontrivial background values of the metric (above extremality)=horizon

and electric potential = CHARGED BLACK HOLE (with flat horizon)

temperature of the dual gauge theory

chemical potential of the dual theory

slide39

The bulk and the boundary in AdS/CFT correspondence

UV/IR: the AdS metric is invariant under

z plays a role of inverse energy scale in 4D theory

z

5D bulk

(+5 internal dimensions)

strings

or supergravity fields

0

gauge fields

4D boundary

computing real time correlation functions from gravity
Computing real-time correlation functions from gravity

To extract transport coefficients and spectral functions from dual gravity,

we need a recipe for computing Minkowski space correlators in AdS/CFT

The recipe of [D.T.Son & A.S., 2001]and [C.Herzog & D.T.Son, 2002] relates

real-time correlators in field theory to Penrose diagram of black hole in dual gravity

Quasinormal spectrum of dual gravity = poles of the retarded correlators in 4d theory

[D.T.Son & A.S., 2001]

slide41

Example: R-current correlator in

in the limit

Zero temperature:

Finite temperature:

Poles of = quasinormal spectrum of dual gravity background

(D.Son, A.S., hep-th/0205051, P.Kovtun, A.S., hep-th/0506184)

slide42

The role of quasinormal modes

G.T.Horowitz and V.E.Hubeny, hep-th/9909056

D.Birmingham, I.Sachs, S.N.Solodukhin, hep-th/0112055

D.T.Son and A.O.S., hep-th/0205052; P.K.Kovtun and A.O.S., hep-th/0506184

I. Computing the retarded correlator: inc.wave b.c. at the horizon, normalized to 1 at the boundary

II. Computing quasinormal spectrum: inc.wave b.c. at the horizon, Dirichlet at the boundary

classification of fluctuations and universality
Classification of fluctuations and universality

O(2) symmetry in x-y plane

Shear channel:

Sound channel:

Scalar channel:

Other fluctuations (e.g. ) may affect sound channel

But not the shear channel

universality of

two point correlation function of stress energy tensor
Two-point correlation function of stress-energy tensor

Field theory

Zero temperature:

Finite temperature:

Dual gravity

  • Five gauge-invariant combinations
  • of and other fields determine
  • obey a system of coupled ODEs
  • Their (quasinormal) spectrum determines singularities

of the correlator

computing transport coefficients from dual gravity various methods
Computing transport coefficients from dual gravity – various methods

1. Green-Kubo formulas (+ retarded correlator from gravity)

2. Poles of the retarded correlators

3. Lowest quasinormal frequency of the dual background

4. The membrane paradigm

slide46

Example: stress-energy tensor correlator in

in the limit

Zero temperature, Euclid:

Finite temperature, Mink:

(in the limit )

The pole

(or the lowest quasinormal freq.)

Compare with hydro:

In CFT:

Also,

(Gubser, Klebanov, Peet, 1996)

slide47

Example 2 (continued): stress-energy tensor correlator in

in the limit

Zero temperature, Euclid:

Finite temperature, Mink:

(in the limit )

The pole

(or the lowest quasinormal freq.)

Compare with hydro:

first order transport coefficients in n 4 sym
First-order transport coefficients in N = 4 SYM

in the limit

Shear viscosity

Bulk viscosity

for non-conformal theories see

Buchel et al; G.D.Moore et al

Gubser et al.

Charge diffusion constant

Supercharge diffusion constant

(G.Policastro, 2008)

Thermal conductivity

Electrical conductivity

slide50

SYM

New transport coefficients in

Sound dispersion:

Kubo:

slide51

Sound and supersymmetric sound in

In 4d CFT

Sound mode:

Supersound mode:

Quasinormal modes in dual gravity

Graviton:

Gravitino:

slide52

Sound dispersion in

analytic approximation

analytic approximation

analytic structure of the correlators
Analytic structure of the correlators

Strong coupling: A.S., hep-th/0207133

Weak coupling: S. Hartnoll and P. Kumar, hep-th/0508092

computing transport coefficients from dual gravity
Computing transport coefficients from dual gravity

Assuming validity of the gauge/gravity duality,

all transport coefficients are completely determined

by the lowest frequencies

in quasinormal spectra of the dual gravitational background

(D.Son, A.S., hep-th/0205051, P.Kovtun, A.S., hep-th/0506184)

This determines kinetics in the regime of a thermal theory

where the dual gravity description is applicable

Transport coefficients and quasiparticle spectra can also be

obtained from thermal spectral functions

shear viscosity in sym
Shear viscosity in SYM

perturbative thermal gauge theory

S.Huot,S.Jeon,G.Moore, hep-ph/0608062

Correction to : Buchel, Liu, A.S., hep-th/0406264

Buchel, 0805.2683 [hep-th]; Myers, Paulos, Sinha, 0806.2156 [hep-th]

electrical conductivity in sym
Electrical conductivity in SYM

Weak coupling:

Strong coupling:

* Charge susceptibility can be computed independently:

D.T.Son, A.S., hep-th/0601157

Einstein relation holds:

universality of
Universality of

Theorem:

For a thermal gauge theory, the ratio of shear viscosity

to entropy density is equal to

in the regime described by a dual gravity theory

Remarks:

  • Extended to non-zero chemical potential:

Benincasa, Buchel, Naryshkin, hep-th/0610145

  • Extended to models with fundamental fermions in the limit

Mateos, Myers, Thomson, hep-th/0610184

  • String/Gravity dual to QCD is currently unknown
universality of shear viscosity in the regime described by gravity duals
Universality of shear viscosity in the regime described by gravity duals

Graviton’s component obeys equation for a minimally

coupled massless scalar. But then .

Since theentropy (density) is

we get

three roads to universality of
Three roads to universality of
  • The absorption argument

D. Son, P. Kovtun, A.S., hep-th/0405231

  • Direct computation of the correlator in Kubo formula from AdS/CFTA.Buchel, hep-th/0408095
  • “Membrane paradigm” general formula for diffusion coefficient + interpretation as lowest quasinormal frequency = pole of the shear mode correlator + Buchel-Liu theorem

P. Kovtun, D.Son, A.S., hep-th/0309213, A.S., 0806.3797 [hep-th],

P.Kovtun, A.S., hep-th/0506184, A.Buchel, J.Liu, hep-th/0311175

a viscosity bound conjecture
A viscosity bound conjecture

Minimum of in units of

P.Kovtun, D.Son, A.S., hep-th/0309213, hep-th/0405231

a hand waving argument
A hand-waving argument

Thus

Gravity duals fix the coefficient:

viscosity entropy ratio of a trapped fermi gas
Viscosity-entropy ratio of a trapped Fermi gas

T.Schafer, cond-mat/0701251

(based on experimental results by Duke U. group, J.E.Thomas et al., 2005-06)

slide65

QCD

Chernai, Kapusta, McLerran, nucl-th/0604032

viscosity measurements at rhic
Viscosity “measurements” at RHIC

Viscosity is ONE of the parameters used in the hydro models

describing the azimuthal anisotropy of particle distribution

  • elliptic flow for
  • particle species “i”

Elliptic flow reproduced for

e.g. Baier, Romatschke, nucl-th/0610108

Perturbative QCD:

Chernai, Kapusta, McLerran, nucl-th/0604032

SYM:

slide67

Elliptic flow with color glass condensate initial conditions

Luzum and Romatschke, 0804.4015 [nuc-th]

slide68

Elliptic flow with Glauber initial conditions

Luzum and Romatschke, 0804.4015 [nuc-th]

slide69

Viscosity/entropy ratio in QCD: current status

Theories with gravity duals in the regime

where the dual gravity description is valid

(universal limit)

Kovtun, Son & A.S; Buchel; Buchel & Liu, A.S

QCD: RHIC elliptic flow analysis suggests

QCD: (Indirect) LQCD simulations

H.Meyer, 0805.4567 [hep-th]

Trapped strongly correlated

cold alkali atoms

T.Schafer, 0808.0734 [nucl-th]

Liquid Helium-3

shear viscosity at non zero chemical potential
Shear viscosity at non-zero chemical potential

Reissner-Nordstrom-AdS black hole

with three R charges

(Behrnd, Cvetic, Sabra, 1998)

(see e.g. Yaffe, Yamada, hep-th/0602074)

J.Mas

D.Son, A.S.

O.Saremi

K.Maeda, M.Natsuume, T.Okamura

We still have

spectral function and quasiparticles in finite temperature ads ir cutoff model
Spectral function and quasiparticles in finite-temperature “AdS + IR cutoff” model
slide72

Photon and dilepton emission

from supersymmetric Yang-Mills plasma

S. Caron-Huot, P. Kovtun, G. Moore, A.S., L.G. Yaffe, hep-th/0607237

slide73

Photon emission from SYM plasma

Photons interacting with matter:

To leading order in

Mimic

by gauging global R-symmetry

Need only to compute correlators of the R-currents

photoproduction rate in sym
Photoproduction rate in SYM

(Normalized) photon production rate in SYM for various values of ‘t Hooft coupling

slide76

Probing quantum liquids with holography

Low-energy elementary

excitations

Specific heat

at low T

Quantum liquid

in p+1 dim

Quantum Bose liquid

phonons

Quantum Fermi liquid

(Landau FLT)

fermionic quasiparticles +

bosonic branch (zero sound)

Departures from normal Fermi liquid occur in

- 3+1 and 2+1 –dimensional systems with strongly correlated electrons

- In 1+1 –dimensional systems for any strength of interaction (Luttinger liquid)

One can apply holography to study strongly coupled Fermi systems at low T

slide77

L.D.Landau (1908-1968)

Fermi Liquid Theory: 1956-58

slide78

The simplest candidate with a known holographic description is

at finite temperature T and nonzero chemical potential associated with the

“baryon number” density of the charge

There are two dimensionless parameters:

is the baryon number density

is the hypermultiplet mass

The holographic dual description in the limit

is given by the D3/D7 system, with D3 branes replaced by the AdS-

Schwarzschild geometry and D7 branes embedded in it as probes.

Karch & Katz, hep-th/0205236

slide79

AdS-Schwarzschild black hole (brane) background

D7 probe branes

The worldvolume U(1) field couples to the flavor current at the boundary

Nontrivial background value of corresponds to nontrivial expectation value of

We would like to compute

- the specific heat at low temperature

- the charge density correlator

slide80

The specific heat (in p+1 dimensions):

(note the difference with Fermi and Bose systems)

The (retarded) charge density correlator

has a pole corresponding to a propagating mode (zero sound)

- even at zero temperature

(note that this is NOT a superfluid phonon whose attenuation scales as )

New type of quantum liquid?

slide81

Other avenues of (related) research

Bulk viscosity for non-conformal theories (Buchel, Gubser,…)

Non-relativistic gravity duals (Son, McGreevy,… )

Gravity duals of theories with SSB (Kovtun, Herzog,…)

Bulk from the boundary (Janik,…)

Navier-Stokes equations and their generalization from gravity (Minwalla,…)

Quarks moving through plasma (Chesler, Yaffe, Gubser,…)

epilogue
Epilogue
  • On the level of theoretical models, there exists a connection
  • between near-equilibrium regime of certain strongly coupled
  • thermal field theories and fluctuations of black holes
  • This connection allows us to compute transport coefficients
  • for these theories
  • At the moment, this method is the only theoretical tool
  • available to study the near-equilibrium regime of strongly
  • coupled thermal field theories
  • The result for the shear viscosity turns out to be universal
  • for all such theories in the limit of infinitely strong coupling
  • Influences other fields (heavy ion physics, condmat)