Thermal spectral functions and holography
Andrei Starinets (Perimeter Institute)
“Strong Fields, Integrability and Strings” program Isaac Newton Institute for Mathematical
Sciences Cambridge, 31.VII.2007
Experimental and theoretical motivation
Heavy ion collision program at RHIC, LHC (2000-2008-2020 ??)
Studies of hot and dense nuclear matter
Abundance of experimental results, poor theoretical understanding:
- the collision apparently creates a fireball of “quark-gluon fluid”
- need to understand both thermodynamics and kinetics
-in particular, need theoretical predictions for parameters entering equations of relativistic hydrodynamics – viscosity etc –
computed from the underlying microscopic theory (thermal QCD)
-this is difficult since the fireball is a strongly interacting nuclear fluid,not a dilute gas
The challenge of RHIC
QCD deconfinement transition (lattice data)
Energy densityvs
temperature
The challenge of RHIC (continued)
Rapid thermalization
Large elliptic flow
Jet quenching
Photon/dilepton emission rates
??
M,J,Q
Holographically dual system in thermal equilibrium
M, J, Q
T S
Gravitational fluctuations Deviations from equilibrium
????
and B.C.
Quasinormal spectrum
10-dim gravity4-dim gauge theory – large N,
strong coupling
+ fluctuations of other fields
Transport (kinetic) coefficients
• Shear viscosity
• Bulk viscosity
• Charge diffusion constant
• Thermal conductivity
• Electrical conductivity
* Expect Einstein relations such as to hold
Gauge/gravity dictionary determines correlators of gauge-invariant operators from gravity
(in the regime where gravity description is valid!)
For example, one can compute the correlators such as
by solving the equations describing fluctuations of the 10-dimgravity background involving AdS-Schwarzschild black hole
Maldacena; Gubser, Klebanov, Polyakov; Witten
Computing finite-temperature correlation functions from gravity
Need to solve 5d e.o.m. of the dual fields propagating in asymptotically AdS space
Can compute Minkowski-space 4d correlators
Gravity maps into real-time finite-temperature formalism (Son and A.S., 2001; Herzog and Son, 2002)
Hydrodynamics: fundamental d.o.f. = densities of conserved charges
Need to add constitutive relations!
Example: charge diffusion
[Fick’s law (1855)]
Conservation law
Constitutive relation
Diffusion equation
Dispersion relation
Expansion parameters:
Similarly, one can analyze another conserved quantity – energy-momentum tensor:
This is equivalent to analyzing fluctuations of energy and pressure
We obtain a dispersion relation for the sound wave:
Hydrodynamics predicts that the retarded correlator
has a “sound wave” pole at
Moreover, in conformal theory
Predictions of hydrodynamics
Now look at the correlators obtained from gravity
The correlator has poles at
The speed of sound coincides with the hydro prediction!
Analytic structure of the correlators
Weak coupling: S. Hartnoll and P. Kumar, hep-th/0508092
Strong coupling: A.S., hep-th/0207133
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)
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
The slope at zero frequency determines the kinetic coefficient Peaks correspond to quasiparticles
Figures show at different values of
Spectral functions and quasiparticles in
Spectral function and quasiparticles in finite-temperature “AdS + IR cutoff”
model
Holographic models with fundamental fermions
Additional parameter makes life more interesting…
Thermal spectral functionsof flavor currents
R.Myers, A.S., R.Thomson, 0706.0162 [hep-th]
Transport coefficients in N=4 SYM
• Shear viscosity
• Bulk viscosity
• Charge diffusion constant
• Thermal conductivity
• Electrical conductivity
in the limit
Shear viscosity in SYM
Correction to : A.Buchel, J.Liu, A.S., hep-th/0406264
perturbative thermal gauge theoryS.Huot,S.Jeon,G.Moore, hep-ph/0608062
Electrical conductivity in SYM
Weak coupling:
Strong coupling:
* Charge susceptibility can be computed independently:
Einstein relation holds:
D.T.Son, A.S., hep-th/0601157
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:
• Extended to models with fundamental fermions in the limit
• String/Gravity dual to QCD is currently unknown
Benincasa, Buchel, Naryshkin, hep-th/0610145
Mateos, Myers, Thomson, hep-th/0610184
A viscosity bound conjecture
P.Kovtun, D.Son, A.S., hep-th/0309213, hep-th/0405231
Minimum of in units of
Chernai, Kapusta, McLerran, nucl-th/0604032
Chernai, Kapusta, McLerran, nucl-th/0604032
Chernai, Kapusta, McLerran, nucl-th/0604032
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)
Chernai, Kapusta, McLerran, nucl-th/0604032
QCD
Viscosity “measurements” at RHIC
Viscosity is ONE of the parameters used in the hydro modelsdescribing the azimuthal anisotropy of particle distribution
-elliptic flow forparticle species “i”
Elliptic flow reproduced for
e.g. Baier, Romatschke, nucl-th/0610108
Perturbative QCD:
SYM:
Chernai, Kapusta, McLerran, nucl-th/0604032
Shear viscosity at non-zero chemical potential
Reissner-Nordstrom-AdS black hole
with three R charges
(Behrnd, Cvetic, Sabra, 1998)
We still have
J.MasD.Son, A.S.O.SaremiK.Maeda, M.Natsuume, T.Okamura
(see e.g. Yaffe, Yamada, hep-th/0602074)
Photon and dilepton emission from supersymmetric Yang-Mills plasmaS. Caron-Huot, P. Kovtun, G. Moore, A.S., L.G. Yaffe, hep-th/0607237
Photons interacting with matter:
Photon emission from SYM plasma
To leading order in
Mimic by gauging global R-symmetry
Need only to compute correlators of the R-currents
Photoproduction rate in SYM
(Normalized) photon production rate in SYM for various values of ‘t Hooft coupling
How far is SYM from QCD?
pQCD (dotted line) vspSYM (solid line)at equal coupling
(and =3)
pQCD (dotted line) vspSYM (solid line)
at equal fermion thermal mass(and =3)
Outlook
Gravity dual description of thermalization ?
Gravity duals of theories with fundamental fermions:
- phase transitions- heavy quark bound states in plasma
- transport properties
Finite ‘t Hooft coupling corrections to photon emission spectrum
Understanding 1/N corrections
Phonino
THE END
Some results
• in the limit described by gravity duals • universal for a large class of theories
Bulk viscosity for non-conformal theories
Shear viscosity/entropy ratio:
• in the limit described by gravity duals • in the high-T regime (but see Buchel et al, to appear…) • model-dependent
R-charge diffusion constant for N=4 SYM:
Non-equilibrium regime of thermal gauge theories is of interest for RHIC and early universe physics
This regime can be studied in perturbation theory, assuming the system is a weakly interacting one. However, this is often NOT the case. Nonperturbative approaches are needed.
Lattice simulations cannot be used directly for real-time processes.
Gauge theory/gravity duality CONJECTURE provides a theoretical tool to probe non-equilibrium, non-perturbative regime of SOME thermal gauge theories
Quantum field theories at finite temperature/density
Equilibrium Near-equilibrium
entropyequation of state
…….
transport coefficientsemission rates
………
perturbative non-perturbative
pQCD Lattice
perturbative non-perturbative
kinetic theory ????
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
The result for the shear viscosity turns out to be universal for all such theories in the limit of infinitely strong coupling
At the moment, this method is the only theoretical tool available to study the near-equilibrium regime of strongly coupled thermal field theories
Stimulating for experimental/theoretical research in other fields
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/CFT A.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., to appear, P.Kovtun, A.S., hep-th/0506184, A.Buchel, J.Liu, hep-th/0311175
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 the entropy (density) is we get
Example 2 (continued): stress-energy tensor correlator in
in the limit
Finite temperature, Mink:
Zero temperature, Euclid:
(in the limit )
The pole (or the lowest quasinormal freq.)
Compare with hydro:
A viscosity bound conjecture
P.Kovtun, D.Son, A.S., hep-th/0309213, hep-th/0405231
Analytic structure of the correlators
Weak coupling: S. Hartnoll and P. Kumar, hep-th/0508092
Strong coupling: A.S., hep-th/0207133
Example 2: stress-energy tensor correlator in
in the limit
Finite temperature, Mink:
Zero temperature, Euclid:
(in the limit )
The pole (or the lowest quasinormal freq.)
Compare with hydro:
In CFT:
Also, (Gubser, Klebanov, Peet, 1996)
Spectral function and quasiparticles
A
B
CA: scalar channel
B: scalar channel - thermal part
C: sound channel
Pressure in perturbative QCD
Quantum field theories at finite temperature/density
Equilibrium Near-equilibrium
entropyequation of state
…….
transport coefficientsemission rates
………
perturbative non-perturbative
pQCD Lattice
perturbative non-perturbative
kinetic theory ????
Thermal spectral functions and holography
Andrei Starinets
“Strong Fields, Integrability and Strings” program Isaac Newton Institute for Mathematical Sciences Cambridge
July 31, 2007
Perimeter Institute for Theoretical Physics
Viscosity “measurements” at RHIC
Viscosity is ONE of the parameters used in the hydro modelsdescribing the azimuthal anisotropy of particle distribution
-elliptic flow forparticle species “i”
Elliptic flow reproduced for
e.g. Baier, Romatschke, nucl-th/0610108
Perturbative QCD:
SYM:
Chernai, Kapusta, McLerran, nucl-th/0604032
A hand-waving argument
Gravity duals fix the coefficient:
Thus
Thermal conductivityNon-relativistic theory:
Relativistic theory:
Kubo formula:
In SYM with non-zero chemical potential
One can compare this with the Wiedemann-Franz lawfor the ratio of thermal to electric conductivity:
Classification of fluctuations and universality
O(2) symmetry in x-y plane
Scalar channel:
Shear channel:
Sound channel:
Other fluctuations (e.g. ) may affect sound channel
But not the shear channel universality of
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 the entropy (density) is we get
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/CFT A.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., to appear, P.Kovtun, A.S., hep-th/0506184, A.Buchel, J.Liu, hep-th/0311175
Effect of viscosity on elliptic flow
Computing transport coefficients from “first principles”
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
Fluctuation-dissipation theory(Callen, Welton, Green, Kubo)
Sound wave pole
Compare:
In CFT: