2015
DOI: 10.1007/jhep05(2015)016
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Holographic thermalization of charged operators

Abstract: We study a light-like charged collapsing shell in AdS-Reissner-Nordstrom spacetime, investigating whether the corresponding Vaidya metric is supported by matter that satisfies the null energy condition. We find that, if the absolute value of the charge decreases during the collapse, energy conditions are fulfilled everywhere in spacetime. On the other hand, if the absolute value of the charge increases, the metric does not satisfy energy conditions in the IR region. Therefore, from the gauge/gravity perspectiv… Show more

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Cited by 12 publications
(15 citation statements)
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References 72 publications
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“…In other words, B = const., as already indicated in (2.32), and 37) for some constant ρ which, from eqs. (2.30)-(2.32) plus (2.40) below, one sees is precisely the U(1) charge density (rescaled by κ),…”
Section: Jhep07(2015)116supporting
confidence: 53%
See 1 more Smart Citation
“…In other words, B = const., as already indicated in (2.32), and 37) for some constant ρ which, from eqs. (2.30)-(2.32) plus (2.40) below, one sees is precisely the U(1) charge density (rescaled by κ),…”
Section: Jhep07(2015)116supporting
confidence: 53%
“…3 Previous work examining thermalization in plasmas with non-zero chemical potential (not involving numerical solutions of far from equilibrium geometries) includes refs. [35][36][37][38].…”
Section: Jhep07(2015)116mentioning
confidence: 99%
“…Readers interested in the results only may want to skip this section. We employ the geodesic approximation as first shown in [18] and used first in asymptotically AdS Vaidya spacetime in [19,20] and subsequently in [22,[25][26][27]65] etc. The Wightman functions are approximated via,…”
Section: Geodesicsmentioning
confidence: 99%
“…to the geodesic of a charged particle accounted for by the introduction of a Lorentz force term [27].…”
Section: Introductionmentioning
confidence: 99%
“…Here, the prime denotes a derivative with respect to v. Equation (28) implies that J λ (ext) J λ(ext) = 0. Hence, the matter current, which sources the gauge field, is null which is permissible for a physical matter current (for related discussions, see [46]).…”
Section: Holographic Thermalization With Weyl Correctionsmentioning
confidence: 99%