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      Firewalls as artefacts of inconsistent truncations of quantum geometries

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          Abstract

          In this paper we argue that a firewall is simply a manifestation of an inconsistent truncation of non-perturbative effects that unitarize the semiclassical black hole. Namely, we show that a naive truncation of quantum corrections to the Hawking spectrum at order \({\cal O}(e^{-S})\), inexorably leads to a "localised'' divergent energy density near the black hole horizon. Nevertheless, in the same approximation, a distant observer only sees a discretised spectrum and concludes that unitarity is achieved by \({\cal O}(e^{-S})\) effects. This is due to the fact that instead, the correct quantum corrections to the Hawking spectrum go like \({\cal O}( g^{tt} e^{-S})\). Therefore, while at a distance far away from the horizon, where \(g^{tt}\approx 1\), quantum corrections {\it are} perturbative, they {\it do} diverge close to the horizon, where \(g^{tt}\rightarrow \infty\). Nevertheless, these "corrections" nicely re-sum so that correlations functions are smooth at the would-be black hole horizon. Thus, we conclude that the appearance of firewalls is just a signal of the breaking of the semiclassical approximation at the Page time, even for large black holes.

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          Holographic representation of local bulk operators

          The Lorentzian AdS/CFT correspondence implies a map between local operators in supergravity and non-local operators in the CFT. By explicit computation we construct CFT operators which are dual to local bulk fields in the semiclassical limit. The computation is done for general dimension in global, Poincare and Rindler coordinates. We find that the CFT operators can be taken to have compact support in a region of the complexified boundary whose size is set by the bulk radial position. We show that at finite N the number of independent commuting operators localized within a bulk volume saturates the holographic bound.
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            Local bulk operators in AdS/CFT: a boundary view of horizons and locality

            We develop the representation of local bulk fields in AdS by non-local operators on the boundary, working in the semiclassical limit and using AdS_2 as our main example. In global coordinates we show that the boundary operator has support only at points which are spacelike separated from the bulk point. We construct boundary operators that represent local bulk operators inserted behind the horizon of the Poincare patch and inside the Rindler horizon of a two dimensional black hole. We show that these operators respect bulk locality and comment on the generalization of our construction to higher dimensional AdS black holes.
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              Information Loss in Black Holes

              S. Hawking (2005)
              The question of whether information is lost in black holes is investigated using Euclidean path integrals. The formation and evaporation of black holes is regarded as a scattering problem with all measurements being made at infinity. This seems to be well formulated only in asymptotically AdS spacetimes. The path integral over metrics with trivial topology is unitary and information preserving. On the other hand, the path integral over metrics with non-trivial topologies leads to correlation functions that decay to zero. Thus at late times only the unitary information preserving path integrals over trivial topologies will contribute. Elementary quantum gravity interactions do not lose information or quantum coherence.
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                Author and article information

                Journal
                2015-02-10
                2015-10-02
                Article
                10.1002/prop.2015000057
                1502.03129
                0ca0eb55-06ec-4f54-974c-330e5fd824eb

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                LMU-ASC 05/15; MPP-2015-19
                Fortschr. Phys. 64, 131 (2016)
                v4: explanation about the failure of the saddle point approximation and general clarifications added
                hep-th gr-qc

                General relativity & Quantum cosmology,High energy & Particle physics
                General relativity & Quantum cosmology, High energy & Particle physics

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