Minkowski-space correlators in AdS/CFT correspondence: recipe and applications

By D. Son, A. Starinets. 2002

1,239 citations recorded by the source corpus.

Subfields: Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/8070ae05469d0e62a3907f17b0ccdc21e3c327cf

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Citations in the corpus

Holographic operator mixing and quasinormal modes on the brane (2009, methodology): “This is so because automatically we can halve the number of basis solutions by demanding “in-going” boundary conditions at this point, which is what leads ultimately to the computation of a retarded Green’s function [2].”
Impure AdS/CFT correspondence (2008, neutral): “Any potential A for this field strength will formally break translation invariance, which is one way to see why GRPP(ω, 0) can be nonzero in the absence of impurities but in the presence of a background magnetic field.”
Pseudogap and time reversal breaking in a holographic superconductor (2008, methodology): “In the recent work [9], the electrical conductivity of a holographic (i.e. AdS/CFT) superconductor was computed as a function of frequency.”
Real-time gauge/gravity duality: prescription, renormalization and examples (2008, methodology): “47) can also be shown to be related to purely ingoing boundary conditions at the horizon [13], leading eventually to the recipe of [12].”
Hydrodynamics of R-charged black holes (2006, methodology): “To compute the correlator, we follow the procedure outlined in [14] and used in [15] to determine the shear viscosity of the strongly coupled N = 4 SYM at zero chemical potential.”
A Bohr-Sommerfeld quantization formula for quasinormal frequencies of AdS black holes (2008, methodology): “In the AdS/CFT correspondence [2,3,4], as a finite temperature boundary gauge theory is described by a black hole in AdS [5], study of quasinormal modes for an AdS black hole is important for understanding dynamics of strongly coupled gauge theories at finite temperature [6,7].”
Nonlinear fluid dynamics from gravity (2007, neutral): “24 56 v4 [ ∗sayanta@theory.tifr.res.in †veronika.hubeny@durham.ac.uk ‡minwalla@theory.tifr.res.in §mukund.rangamani@durham.ac.uk Contents”
The Hydrodynamics of M-Theory (2002, methodology): “The “incoming wave” boundary condition described in [4] forces us to choose α = −iω5/3.”
Introduction to Holographic Superconductors (2010, neutral): “, yields the retarded Green’s function [55].”
Momentum fluctuations of heavy quarks in the gauge-string duality (2006, methodology): “In [44] a restriction was made to consider only diagonal metrics, so the question of including dependence of the wave-function on coordinates other than the radial one never arose.”
Overdamped modes in Schwarzschild-de Sitter and a Mathematica package for the numerical computation of quasinormal modes (2017, background): “the gravity side corresponds a gauge-invariant operator on the QFT side. The quasinormal frequencies of this eld are equal to the poles in the retarded Green’s function of the operator in the dual QFT[9,12]. By summing quasinormal modes one can compute one loop determinants[20]. Out of equilibrium g”
Schwinger-Keldysh propagators from AdS/CFT correspondence (2002, background): “In (1+1)-dimensional conformal field theory where the Euclidean Green’s function can be computed exactly and the analytic continuation to a Minkowski signature metric can be performed, the prescription gives the correct GR [9].”