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![Page 1: Gauge/gravity duality and transport in hot and dense nuclear matter Andrei Starinets Oxford Elementary Particle Physics Seminars 11 November 2008 Rudolf.](https://reader030.fdocuments.in/reader030/viewer/2022032600/56649db95503460f94aa8ed1/html5/thumbnails/1.jpg)
Gauge/gravity duality and
transport in hot and dense nuclear matter
Andrei Starinets
Oxford Elementary Particle Physics Seminars
11 November 2008
Rudolf Peierls Centre for Theoretical Physics
Oxford University
![Page 2: Gauge/gravity duality and transport in hot and dense nuclear matter Andrei Starinets Oxford Elementary Particle Physics Seminars 11 November 2008 Rudolf.](https://reader030.fdocuments.in/reader030/viewer/2022032600/56649db95503460f94aa8ed1/html5/thumbnails/2.jpg)
Heavy ion collision experiments at RHIC (2000-current) and LHC (2009-??)create hot and dense nuclear matter known as the “quark-gluon plasma”
Evolution of the plasma “fireball” is described by relativistic fluid dynamics
(note: qualitative difference between p-p and Au-Au collisions)
Need to know
thermodynamics (equation of state) kinetics (first- and second-order transport coefficients)in the regime of intermediate coupling strength:
(relativistic Navier-Stokes equations)
initial conditions (initial energy density profile)
thermalization time (start of hydro evolution)
freeze-out conditions (end of hydro evolution)
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AdS/CFT
heavy-ion physics
condensed matter physics
thermal QCD
non-relativistic AdS/CFT
black hole physics
AdS/QCD
quantum liquids
technicolor
relativistic hydrodynamics
quantum gravity
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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 ????
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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
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Figure: an artistic impression from Myers and Vazquez, 0804.2423 [hep-th]
Energy density vs temperature for various gauge theories
Ideal gasof quarksand gluons
Ideal gasof hadrons
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The challenge of RHIC (continued)
Rapid thermalization
Large elliptic flow
Jet quenching
Photon/dilepton emission rates
??
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First-order transport (kinetic) coefficients
* Expect Einstein relations such as to hold
Shear viscosity
Bulk viscosity
Charge diffusion constant
Supercharge diffusion constant
Thermal conductivity
Electrical conductivity
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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:
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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
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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
conjecturedexact equivalence
Maldacena (1997); Gubser, Klebanov, Polyakov (1998); Witten (1998)
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AdS/CFT correspondence
conjecturedexact equivalence
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
Latest test: Janik’08
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4D boundary
z
0
The bulk and the boundary in AdS/CFT correspondence
5D bulk (+5 internal dimensions)
UV/IR: the AdS metric is invariant under
z plays a role of inverse energy scale in 4D theory
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supersymmetric Yang-Mills is the harmonic oscillator of the XXI century!
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• Field content:
• Action:
Gliozzi,Scherk,Olive’77
Brink,Schwarz,Scherk’77
(super)conformal field theory = coupling doesn’t run
supersymmetric YM theory
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AdS/CFT correspondence is the simplest example of the gauge/string (gauge/gravity) duality
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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)
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Computing transport coefficients from dual gravity
Assuming validity of the gauge/gravity duality, all transport coefficients are completely determined
by the lowest frequenciesin quasinormal spectra of the dual gravitational background
This determines kinetics in the regime of a thermal theorywhere the dual gravity description is applicable
(D.Son, A.S., hep-th/0205051, P.Kovtun, A.S., hep-th/0506184)
Transport coefficients and quasiparticle spectra can also beobtained from thermal spectral functions
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First-order transport coefficients in N = 4 SYM in the limit
Shear viscosity
Bulk viscosity
Charge diffusion constant
Supercharge diffusion constant
Thermal conductivity
Electrical conductivity
(G.Policastro, 2008)
for non-conformal theories see Buchel et al; G.D.Moore et al Gubser et al.
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Shear viscosity in SYM
Correction to : Buchel, Liu, A.S., hep-th/0406264
perturbative thermal gauge theoryS.Huot,S.Jeon,G.Moore, hep-ph/0608062
Buchel, 0805.2683 [hep-th]; Myers, Paulos, Sinha, 0806.2156 [hep-th]
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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
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Spectral function and quasiparticles
A
B
CA: scalar channel
B: scalar channel - thermal part
C: sound channel
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Universality of
Theorem:
For any thermal gauge theory (with zero chemicalpotential), the ratio of shear viscosity to entropy density is equal to in the regime describedby a corresponding 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
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A viscosity bound conjecture
P.Kovtun, D.Son, A.S., hep-th/0309213, hep-th/0405231
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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
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Luzum and Romatschke, 0804.4015 [nuc-th]
Elliptic flow with color glass condensate initial conditions
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Luzum and Romatschke, 0804.4015 [nuc-th]
Elliptic flow with Glauber initial conditions
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Viscosity/entropy ratio in QCD: current status
QCD: RHIC elliptic flow analysis suggests
Theories with gravity duals in the regimewhere the dual gravity description is valid
(universal limit)
QCD: (Indirect) LQCD simulations
H.Meyer, 0805.4567 [hep-th]
Trapped strongly correlated cold alkali atoms
Liquid Helium-3
T.Schafer, 0808.0734 [nucl-th]
Kovtun, Son & A.S; Buchel; Buchel & Liu, A.S
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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)
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Photon and dilepton emission from supersymmetric Yang-Mills plasmaS. Caron-Huot, P. Kovtun, G. Moore, A.S., L.G. Yaffe, hep-th/0607237
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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
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Photoproduction rate in SYM
(Normalized) photon production rate in SYM for various values of ‘t Hooft coupling
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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
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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
Influences other fields (heavy ion physics, condmat)
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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
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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
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Analytic structure of the correlators
Weak coupling: S. Hartnoll and P. Kumar, hep-th/0508092
Strong coupling: A.S., hep-th/0207133
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Pressure in perturbative QCD
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A hand-waving argument
Gravity duals fix the coefficient:
Thus
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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:
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Effect of viscosity on elliptic flow