2016
DOI: 10.1007/jhep08(2016)177
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Aspects of holographic entanglement at finite temperature and chemical potential

Abstract: Abstract:We investigate the behavior of entanglement entropy at finite temperature and chemical potential for strongly coupled large-N gauge theories in d-dimensions (d ≥ 3) that are dual to Anti-de Sitter-Reissner-Nordstrom geometries in (d + 1)−dimensions, in the context of gauge-gravity duality. We develop systematic expansions based on the RyuTakayanagi prescription that enable us to derive analytic expressions for entanglement entropy and mutual information in different regimes of interest. Consequently, … Show more

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Cited by 55 publications
(118 citation statements)
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References 78 publications
(167 reference statements)
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“…The previous studies [8,12,13,15,16] which used the AdS-Reissner-Nordstrom geometry as the model spacetime is not the external field. The EM fields therein are used to form the black hole itself and dual to the field theory in the present of chemical potential.…”
Section: Jhep02(2017)032mentioning
confidence: 99%
“…The previous studies [8,12,13,15,16] which used the AdS-Reissner-Nordstrom geometry as the model spacetime is not the external field. The EM fields therein are used to form the black hole itself and dual to the field theory in the present of chemical potential.…”
Section: Jhep02(2017)032mentioning
confidence: 99%
“…The resulting quantity is thus finite. Following [27,28], let us now consider two separate limits: (i) u c u * and (ii) u c ∼ u * . Case (i), in which the geodesic stays mostly away from the infrared horizon, is equivalent to taking l/u * = l √ E 1.…”
Section: General Geodesicsmentioning
confidence: 99%
“…Considering large entangling region limit, i.e., ρ h , the main contribution to the area of the minimal surface comes from the limit where it is extended all the way to the horizon, such that ρ t ∼ ρ h (see [35][36][37] for related analysis). In this limit by defining ρ = ρ t ξ, one finds…”
Section: Jhep10(2016)135mentioning
confidence: 99%