From AdS/CFT correspondence to hydrodynamics. II. Sound waves

By Giuseppe Policastro, D. Son, A. Starinets. 2002

177 citations recorded by the source corpus.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics

View Paper: https://www.semanticscholar.org/paper/8a604fa457b9ddb36ed71670e1c09d64d08e690e

How researchers see this paper

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In Astronomy and Astrophysics

1. M. Rangamani
2. S. Hartnoll
3. V. Hubeny
4. P. Kovtun
5. A. Yarom
6. D. Mateos
7. A. Starinets
8. S. Sachdev

In Nuclear and High Energy Physics

1. M. Rangamani
2. S. Hartnoll
3. V. Hubeny
4. P. Kovtun
5. R. Myers
6. D. Mateos
7. A. Yarom
8. M. Kaminski

Citations in the corpus

• Lectures on holographic methods for condensed matter physics (2009, methodology): “[86] for uses of Ward identities in this manner).”
• Lectures on hydrodynamic fluctuations in relativistic theories (2012, background): “ly theoretical physics point of view. It turns out that hydrodynamic fluctuations (both in normal fluids and in superfluids) can be thought of as gravitational fluctuations of black holes, and vice versa [3, 4]. In fact, this connection between gravity and hydrodynamics works beyond the linear response,”
• The fluid/gravity correspondence: a new perspective on the membrane paradigm (2010, unknown): “Such modes with hydrodynamic dispersion relations were first considered in [41, 42] and describe a propagating sound mode with linear dispersion and shear mode with damped quadratic dispersion.”
• Gravity and hydrodynamics: lectures on the fluid-gravity correspondence (2009, background): “zed fluid dynamics from linearized gravity in asymptotically AdS black hole backgrounds. The exploration of linearized hydrodynamics has been carried out in various different contexts over the years in [19, 27, 28, 29, 30, 31, 32, 33, 34, 35, 36, 37, 38, 39, 40, 41, 42, 43] and we refer the reader to ”
• String theory and quantum chromodynamics (2007, background): “It is remarkable that strongly coupled plasmas with a gravity dual generically exhibit no peaks of this type, but only peaks associated to hydrodynamic modes and peaks whose width is comparable to their height [ 35 , 36].”
• Transport properties of the quark-gluon plasma (2011, methodology): “ir analytic structure with the analytic structure found at weak coupling using kinetic theory. For the interested reader, the method of computing spectral functions based on the holographic principle [77,78,79,80,56] has been reviewed in [81,49,50]. The spectral function of the R-charge correlator a”
• AdS / CFT correspondence, quasinormal modes, and thermal correlators in N=4 SYM (2003, methodology): “This means that none of the N = 4 SYM operators dual to massive scalar fields exhibits hydrodynamic behavior similar to the one described in [5], [6].”
• Parity-violating hydrodynamics in 2 + 1 dimensions (2011, background): “ , (4.3b) where is the grand canonical density operator specifying the equilibrium state of the system. The retarded functions defined by (4.2) and (4.3) will differ by contact terms. See for example [55,56] for a discussion. In the remainder of this subsection we will study general properties of the”