2016
DOI: 10.1007/jhep11(2016)028
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Deriving covariant holographic entanglement

Abstract: We provide a gravitational argument in favour of the covariant holographic entanglement entropy proposal. In general time-dependent states, the proposal asserts that the entanglement entropy of a region in the boundary field theory is given by a quarter of the area of a bulk extremal surface in Planck units. The main element of our discussion is an implementation of an appropriate Schwinger-Keldysh contour to obtain the reduced density matrix (and its powers) of a given region, as is relevant for the replica c… Show more

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Cited by 260 publications
(392 citation statements)
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References 74 publications
(329 reference statements)
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“…A covariant version was proposed by Hubeny, Rangamani and Takayanagi (HRT) [59]. Using AdS/CFT for Einstein gravity, RT and HRT proposal have been proved by [60][61][62][63][64]. It is interesting to ask if the connection between spacetime structure in the bulk and entanglement in the boundary still exist beyond the context of AdS/CFT, and if so, how it works for non-AlAdS spacetimes.…”
Section: Jhep07(2017)142mentioning
confidence: 99%
See 2 more Smart Citations
“…A covariant version was proposed by Hubeny, Rangamani and Takayanagi (HRT) [59]. Using AdS/CFT for Einstein gravity, RT and HRT proposal have been proved by [60][61][62][63][64]. It is interesting to ask if the connection between spacetime structure in the bulk and entanglement in the boundary still exist beyond the context of AdS/CFT, and if so, how it works for non-AlAdS spacetimes.…”
Section: Jhep07(2017)142mentioning
confidence: 99%
“…The second approach is to directly propose a prescription in the bulk, and check its consistency [70,71]. The third approach, which we will advocated in the current paper, is to derive an analog of RT proposal using the dictionary of holography, along the lines of [60][61][62][63][64]. In [72,73], holographic entanglement entropy in Warped AdS 3 spacetime was derived by generalizing the gravitational entropy [63] and Rindler method [60,74], respectively.…”
Section: Jhep07(2017)142mentioning
confidence: 99%
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“…However the tensor networks designed in [24,25] only consider the geometry of a spatial slice in AdS, without any input about time evolution. In the continuum AdS/CFT context, the correct entanglement spectrum are obtained by considering the spacetime geometry, and taking into account the bulk dynamics given by the Einstein equation [11,12,14,15], while [24,25] don't have any dynamical input. In this work, we take the above idea as a hint to improve the random tensor network approach, in which we resolve the issue.…”
Section: Jhep11(2017)148mentioning
confidence: 99%
“…This includes the (leading order) holographic mutual information defined by the Ryu-Takayanagi (RT) [11,12] or the covariant Hubeny-RangamaniTakayanagi (HRT) [13] prescriptions. While -as will be discussed in section 4 -the derivations of [14] and [15] need not apply to our spacetime, it is nevertheless of interest to investigate what these prescriptions would predict. In particular, we will see thatdespite the instability noted above -in a sense these mutual informations (and indeed the entropies of all boundary regions) appear to already be thermalized at any finite t.…”
Section: Mutual Information and Thermalizationmentioning
confidence: 99%