Real‐time response in AdS/CFT with application to spinors
271 citations recorded by the source corpus.
We discuss a simple derivation of the real‐time AdS/CFT prescription as an analytic continuation of the corresponding problem in Euclidean signature. We then extend the formalism to spinor operators and apply it to the examples of real‐time fermionic correlators in CFTs dual to pure AdS and the BTZ black hole.
Subfields: Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/807aaa15d1e98f0a038c89a81afa20a4fc41e951
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In Nuclear and High Energy Physics
In Statistical and Nonlinear Physics
Citations in the corpus
- Peculiar properties of a charged dilatonic black hole in AdS 5 (2009, background): “These normal modes correspond to poles of the retarded Green’s function [22], with normal modes with nonzero u1 (or nonzero u + 2 ) corresponding to poles of G11 (or poles of G22, resp.”
- Strongly correlated quantum fluids: ultracold quantum gases, quantum chromodynamic plasmas and holographic duality (2012, background): “The basic strategy can be found in [349, 350, 351, 237, 339].”
- Lectures on holographic non-Fermi liquids and quantum phase transitions (2011, methodology): “We refer readers to [38, 40, 83] for detailed analysis of the Dirac equation and only mention the main results here.”
- Holographic Duality with a View Toward Many-Body Physics (2009, background): “This formula applies in the real-time case [47].”
- A Holographic View on Physics out of Equilibrium (2010, background): “More recently, these arguments have been revisited in [58] and a compact expression for computing two-point functions was provided in [59, 60].”
- Gauge gravity duality for d-wave superconductors: prospects and challenges (2010, methodology): “The prescription to compute the retarded Green’s function is then [45]”
- ABJ triality: from higher spin fields to strings (2012, methodology): “[26]) that the AdS/CFT dictionary for such fermions identifies the ‘source’ with the coefficient of the z 3 2 fall off of the parity even part of the bulk fermionic field (the same information is also present in the z 5 2 fall off of the parity odd part of the fermion field), while the ‘operator vev”
- Holographic Quantum Matter (2016, background): “We can now be more precise – see [410; 564] for more details on the following.”