2017
DOI: 10.1007/jhep04(2017)134
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No simple dual to the causal holographic information?

Abstract: In AdS/CFT, the fine grained entropy of a boundary region is dual to the area of an extremal surface X in the bulk. It has been proposed that the area of a certain 'causal surface' C-i.e. the 'causal holographic information' (CHI)corresponds to some coarse-grained entropy in the boundary theory. We construct two kinds of counterexamples that rule out various possible duals, using (1) vacuum rigidity and (2) thermal quenches. This includes the 'one-point entropy' proposed by Kelly and Wall, and a large class of… Show more

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Cited by 19 publications
(32 citation statements)
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References 94 publications
(171 reference statements)
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“…In previous work, we showed that the outer entropy of a slice of the event horizon is not, in general, given by its area [21]; in fact in some situations the outer entropy vanishes, while the area of the event horizon does not. Although the area of the event horizon is generically greater than the HRT surface [22], it remains unclear what coarse graining procedure, if any, corresponds to its area [23,24].…”
Section: Ow[σ]mentioning
confidence: 92%
“…In previous work, we showed that the outer entropy of a slice of the event horizon is not, in general, given by its area [21]; in fact in some situations the outer entropy vanishes, while the area of the event horizon does not. Although the area of the event horizon is generically greater than the HRT surface [22], it remains unclear what coarse graining procedure, if any, corresponds to its area [23,24].…”
Section: Ow[σ]mentioning
confidence: 92%
“…for Minkowski, AdS, and dS. This conclusion follows in general in the Minkowski case from the positive mass theorem[30,31] and in the (A)dS cases from its generalization to spacetimes that are not asymptotically flat; see Ref [32]. for an AdS/CFT perspective 13.…”
mentioning
confidence: 82%
“…We can also define an entropy associated with a more general subset of observables that does not necessarily form a subalgebra. 9 Entropies of this type have been discussed previously in the context of holography in [39][40][41]. Given a set of (not necessarily commuting) operators A = {O α } and a global state ρ, we can look for a state ρ A that maximizes the von Neumann entropy subject to the constraint that…”
Section: Entropy Associated With a Subset Of Observablesmentioning
confidence: 99%