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Gauge-Gravity Duality: A brief overview Andrei Starinets ICMS workshop Numerical relativity beyond astrophysics Edinburgh 12 July 2011 Rudolf Peierls Centre for Theoretical Physics Oxford University

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Some references: O.Aharony, S.Gubser, J.Maldacena, H.Ooguri, Y.Oz, hep-th/ P.K.Kovtun and A.O.S., Quasinormal modes and holography, hep-th/ D.T.Son and A.O.S., Viscosity, Black Holes, and Quantum Field Theory, [hep-th] J.Casalderrey-Solana, H.Liu, D.Mateos, K.Rajagopal, U.Wiedemann, [hep-th]

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S. Hartnoll Lectures on holographic methods for condensed matter physics, [hep-th] C. Herzog Lectures on holographic superfluidity and superconductivity, [hep-th] M. Rangamani Gravity and hydrodynamics: Lectures on the fluid-gravity correspondence, [hep-th] AdS/CFT and condensed matter physics S.Sachdev Condensed matter and AdS/CFT, [hep-th]

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What is string theory?

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Equations such as describe the low energy limit of string theory As long as the dilaton is small, and thus the string interactions are suppressed, this limit corresponds to classical 10-dim Einstein gravity coupled to certain matter fields such as Maxwell field, p-forms, dilaton, fermions Validity conditions for the classical (super)gravity approximation - curvature invariants should be small: - quantum loop effects (string interactions = dilaton) should be small: In AdS/CFT duality, these two conditions translate into and

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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 conjectured exact equivalence Maldacena (1997); Gubser, Klebanov, Polyakov (1998); Witten (1998)

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Field content: Action: Gliozzi,Scherk,Olive77 Brink,Schwarz,Scherk77 (super)conformal field theory = coupling doesnt run supersymmetric YM theory

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AdS/CFT correspondence conjectured exact 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

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AdS/CFT correspondence: the role of J satisfies linearized supergravity e.o.m. with b.c. For a given operator, identify the source field, e.g. 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. Then, taking functional derivatives of gives The recipe: Warning: e.o.m. for different bulk fields may be coupled: need self-consistent solution

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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

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Hydrodynamics: fundamental d.o.f. = densities of conserved charges Need to add constitutive relations! Example: charge diffusion [Ficks 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 background fluctuations Deviations from equilibrium ???? and B.C. Quasinormal spectrum 10-dim gravity 4-dim gauge theory – large N, strong coupling

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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 is an effective theory, valid for sufficiently small momenta First-order hydro eqs are parabolic. They imply instant propagation of signals. Second-order hydrodynamics 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)

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Second-order conformal hydrodynamics (in d dimensions)

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Second-order transport (kinetic) coefficients Relaxation time Second order trasport coefficient (for theories conformal at T=0) In non-conformal theories such as QCD, the total number of second-order transport coefficients is quite large

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Predictions of the second-order conformal hydrodynamics Sound dispersion: Kubo:

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In quantum field theory, the dispersion relations such as appear as poles of the retarded correlation functions, e.g. - in the hydro approximation -

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The role of quasinormal modes G.T.Horowitz and V.E.Hubeny, hep-th/ D.Birmingham, I.Sachs, S.N.Solodukhin, hep-th/ D.T.Son and A.O.S., hep-th/ ; P.K.Kovtun and A.O.S., hep-th/ 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

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Sound and supersymmetric sound in Sound mode: Supersound mode: In 4d CFT Quasinormal modes in dual gravity Graviton: Gravitino:

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Quasinormal spectra of black holes/branes Schwarzschild black hole (asymptotically flat) AdS-Schwarzschild black brane

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Sound dispersion in analytic approximation

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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/ perturbative thermal gauge theory S.Huot,S.Jeon,G.Moore, hep-ph/ Buchel, [hep-th]; Myers, Paulos, Sinha, [hep-th]

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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/ Mateos, Myers, Thomson, hep-th/

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Three roads to universality of The absorption argument D. Son, P. Kovtun, A.S., hep-th/ Direct computation of the correlator in Kubo formula from AdS/CFT A.Buchel, hep-th/ 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/ , A.S., [hep-th], P.Kovtun, A.S., hep-th/ , A.Buchel, J.Liu, hep-th/

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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 frequencies in quasinormal spectra of the dual gravitational background This determines kinetics in the regime of a thermal theory where the dual gravity description is applicable (D.Son, A.S., hep-th/ , P.Kovtun, A.S., hep-th/ ) Transport coefficients and quasiparticle spectra can also be obtained from thermal spectral functions

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Hydrodynamic properties of strongly interacting hot plasmas in 4 dimensions can be related (for certain models!) to fluctuations and dynamics of 5-dimensional black holes

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Beyond near-equilibrium regime

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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]

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