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Related papers: Behind the Horizon in AdS/CFT

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We study the emission rates of scalar, spinor and vector particles from a 5 dimensional black hole for arbitrary partial waves. The solution is lifted to 6 dimensions, and the near horizon $ BTZ \times S^3$ geometry of the black hole…

High Energy Physics - Theory · Physics 2014-11-18 Saurya Das , Arundhati Dasgupta

We consider the massless BTZ black hole and show that it is possible to take its "near horizon" limit in two distinct ways. The first one leads to a null self-dual orbifold of AdS3 and the second to a spacelike singular AdS3/Z_K orbifold in…

High Energy Physics - Theory · Physics 2011-08-17 Jan de Boer , M. M. Sheikh-Jabbari , Joan Simon

The microscopic origin of black hole entropy remains one of the more intriguing open questions in theoretical physics. A subplot in this drama is the renowned Cardy-Verlinde formula, which uses two-dimensional conformal formalism to explain…

High Energy Physics - Theory · Physics 2007-05-23 A. J. M. Medved

Using the D1D5 CFT we investigate transitions involving a member of a certain class of states called superstrata states, which are holographically dual to certain smooth, horizonless, $1/8$-BPS, three-charge black hole microstates known as…

High Energy Physics - Theory · Physics 2025-02-26 Shaun D. Hampton

Two dimensional charged black holes in string theory can be obtained as exact (SL(2,R)xU(1))/U(1) quotient CFTs. The geometry of the quotient is induced from that of the group, and in particular includes regions beyond the black hole…

High Energy Physics - Theory · Physics 2009-11-10 Amit Giveon , Eliezer Rabinovici , Amit Sever

We study the dual description of the self-dual orbifold, a locally AdS_3 spacetime which is a circle fibration over AdS_2 and arises as the near-horizon limit of the extreme BTZ black hole. The geometry has two boundaries; we argue that…

High Energy Physics - Theory · Physics 2011-06-21 Vijay Balasubramanian , Jamie Parsons , Simon F. Ross

We consider the algebra of simple operators defined in a time band in a CFT with a holographic dual. When the band is smaller than the light crossing time of AdS, an entire causal diamond in the center of AdS is separated from the band by a…

High Energy Physics - Theory · Physics 2016-05-25 Souvik Banerjee , Jan-Willem Bryan , Kyriakos Papadodimas , Suvrat Raju

In this paper we extend the HKLL holographic smearing function method to reconstruct (quasi)local AdS bulk scalar observables in the background of a large AdS black hole formed by null shell collapse (a "pure state" black hole), from the…

High Energy Physics - Theory · Physics 2015-12-16 Shubho R. Roy , Debajyoti Sarkar

To gain insight into how bulk locality emerges from the holographic conformal field theory, we reformulate the bulk to boundary map in as local a way as possible. In previous work, we carried out this program for Lorentzian AdS, and showed…

High Energy Physics - Theory · Physics 2014-11-18 Alex Hamilton , Daniel Kabat , Gilad Lifschytz , David A. Lowe

Large black holes in an asymptotically AdS spacetime have a dual description in terms of approximately thermal states in the boundary CFT. The reflecting boundary conditions of AdS prevent such black holes from evaporating completely. On…

High Energy Physics - Theory · Physics 2008-11-26 Jorge V. Rocha

We analytically calculate the quasi-normal modes of various perturbations of spacelike stretched and null warped $AdS_3$ black holes. From AdS/CFT correspondence, these quasi-normal modes are expected to appear as the poles in momentum…

High Energy Physics - Theory · Physics 2010-02-08 Bin Chen , Zhi-bo Xu

For a given conformal field theory (CFT), one can deform it via the addition of a marginal operator to the spectrum. In two dimensions, when the added operator has conformal weights $h=\bar{h}=1$, conformal symmetry is not broken and the…

High Energy Physics - Theory · Physics 2025-11-27 Michael Imseis , Sruthi A. Narayanan , A. W. Peet

The central dogma of black hole physics -- which says that from the outside a black hole can be described in terms of a quantum system with exp$(\text{Area}/4G_N)$ states evolving unitarily -- has recently been supported by computations…

High Energy Physics - Theory · Physics 2022-02-09 Edgar Shaghoulian

We analyze the near-horizon limit of a general black hole with two commuting killing vector fields in the limit of zero temperature. We use black hole thermodynamics methods to relate asymptotic charges of the complete spacetime to those…

High Energy Physics - Theory · Physics 2014-11-21 Bruno Carneiro da Cunha , Amilcar R. de Queiroz

We argue that, given the nonlocal nature of precursors in AdS/CFT correspondence, the boundary field theory contains information about events inside a black hole horizon. The essence of our proposal is sketched in figure 1, and relies on…

High Energy Physics - Theory · Physics 2009-11-07 Veronika E. Hubeny

We present a generalisation of the embedding space formalism to conformal field theories (CFTs) on non-trivial states and curved backgrounds, based on the ambient metric of Fefferman and Graham. The ambient metric is a Lorentzian Ricci-flat…

High Energy Physics - Theory · Physics 2023-04-05 Enrico Parisini , Kostas Skenderis , Benjamin Withers

In the paper we further refine the thermodynamics method of black hole/CFT correspondence. We show that one can derive the central charges of different holographic pictures directly from the entropy product $S_+S_-$ if it is…

High Energy Physics - Theory · Physics 2013-04-04 Bin Chen , Zhao Xue , Jia-ju Zhang

Effective theories are being developed for fields outside black holes, often with an unusual open-system feel due to the influence of large number of degrees of freedom that lie out of reach beyond the horizon. What is often difficult when…

High Energy Physics - Theory · Physics 2021-09-08 G. Kaplanek , C. P. Burgess , R. Holman

We investigate the description of the region behind the event horizon in rotating black holes in the AdS/CFT correspondence, using the rotating BTZ black hole as a concrete example. We extend a technique introduced by Kraus, Ooguri and…

High Energy Physics - Theory · Physics 2009-11-10 Thomas S. Levi , Simon F. Ross

In Lorentzian AdS/CFT there exists a mapping between local bulk operators and nonlocal CFT operators. In global AdS this mapping can be found through use of bulk equations of motion and allows the nonlocal CFT operator to be expressed as a…

High Energy Physics - Theory · Physics 2013-08-15 Stefan Leichenauer , Vladimir Rosenhaus
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