2012
DOI: 10.1088/0264-9381/29/23/235025
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Abstract: In this note, we explain how asymptotically globally AdS spacetimes can be given an alternate dual description as entangled states of a pair of hyperbolic space CFTs, which are associated with complementary Rindler

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Cited by 91 publications
(126 citation statements)
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“…This happens for k = 0 at a single point on S d−1 , whereas the infinite injection of energy occurs in the k = −1 case along the complete equatorial S d−2 which separates S d−1 into two hemispheres. It follows that singularities of 'firewall' type are expected in the global bulk description of such states, in agreement with the philosophy expressed in [42,43]. The price we pay for the ability to use a classical set up is the need to realize the state in a CFT perturbed by a large relevant operator, but the take-away message ends up being the same.…”
Section: Jhep12(2013)023supporting
confidence: 72%
“…This happens for k = 0 at a single point on S d−1 , whereas the infinite injection of energy occurs in the k = −1 case along the complete equatorial S d−2 which separates S d−1 into two hemispheres. It follows that singularities of 'firewall' type are expected in the global bulk description of such states, in agreement with the philosophy expressed in [42,43]. The price we pay for the ability to use a classical set up is the need to realize the state in a CFT perturbed by a large relevant operator, but the take-away message ends up being the same.…”
Section: Jhep12(2013)023supporting
confidence: 72%
“…Thus, they argue that an infalling observer will experience a firewall (if the assumptions hold). 1 Firewalls were also proposed in a different context in [43], following [44][45][46][47][48][49][50][51][52][53]. There, in the nonperturbative setting of AdS/CFT, it was argued that the existence of any spacetime at all behind a general horizon (including Rindler horizons in pure AdS) requires entanglement between the degrees of freedom associated with the region outside the horizon and some other independent degrees of freedom (see figure 1).…”
Section: Introductionmentioning
confidence: 99%
“…The reason to ask this question is because there are many different quantum states in H L ⊗ H R giving rise to the same density matrix ρ R capturing the physics of a single asymptotic observer. This suggests that ρ R only describes the exterior of the AdS event horizon [42][43][44][45].…”
Section: Jhep06(2014)038mentioning
confidence: 99%