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Related papers: Excitations in the deformed D1D5 CFT

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We are interested in thermalization in the D1D5 CFT, since this process is expected to be dual to black hole formation. We expect that the lowest order process where thermalization occurs will be at second order in the perturbation that…

High Energy Physics - Theory · Physics 2017-12-06 Zaq Carson , Shaun Hampton , Samir D. Mathur

The D1D5 CFT gives a holographic dual description of a near-extremal black hole in string theory. The interaction in this theory is given by a marginal deformation operator, which is composed of supercharges acting on a twist operator. The…

High Energy Physics - Theory · Physics 2015-02-24 Zaq Carson , Shaun Hampton , Samir D. Mathur , David Turton

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

Thermalization in the D1D5 CFT should occur via interactions caused by the twist operator, which deforms the theory off its free orbifold point. Earlier studies investigating this deformation at first order did not show any definite…

High Energy Physics - Theory · Physics 2017-08-21 Zaq Carson , Shaun Hampton , Samir D. Mathur

The D1D5 CFT has been very useful in the study of black holes. The interaction in this theory involves a twist operator, which links together different copies of a free CFT. For the bosonic fields, we examine the action of this twist when…

High Energy Physics - Theory · Physics 2014-10-31 Zaq Carson , Shaun Hampton , Samir D. Mathur , David Turton

We consider the issue of thermalization in the D1D5 CFT. Thermalization is expected to correspond to the formation of a black hole in the dual gravity theory. We start from the orbifold point, where the theory is essentially free, and does…

High Energy Physics - Theory · Physics 2017-08-18 Zaq Carson , Shaun Hampton , Samir D. Mathur

The free orbifold point of the D1-D5 CFT must be deformed with a scalar marginal operator driving it to the region in moduli space where the holographic supergravity description of fuzzball microstates becomes available. We discuss the…

High Energy Physics - Theory · Physics 2021-12-22 Andre Alves Lima , Galen M. Sotkov , Marian Stanishkov

We consider states of the D1-D5 CFT where only the left-moving sector is excited. As we deform away from the orbifold point, some of these states will remain BPS while others can `lift'. We compute this lifting for a particular family of…

High Energy Physics - Theory · Physics 2019-01-30 Shaun Hampton , Samir D. Mathur , Ida G. Zadeh

We consider D1-D5-P states in the untwisted sector of the D1-D5 orbifold CFT where one copy of the seed CFT has been excited by a pair of oscillators, each being either bosonic or fermionic. While such states are BPS at the orbifold point,…

High Energy Physics - Theory · Physics 2023-10-24 Marcel R. R. Hughes , Samir D. Mathur , Madhur Mehta

The D1D5 CFT has provided a useful microscopic model for studying black holes. The coupling in this theory is a twist deformation whose action on the vacuum generates a squeezed state. We give a new derivation of the expression for this…

High Energy Physics - Theory · Physics 2015-07-08 Benjamin A. Burrington , Samir D. Mathur , Amanda W. Peet , Ida G. Zadeh

In this dissertation, we review work presented in arXiv:0906.2015, arXiv:0907.1663, arXiv:1002.3132, arXiv:1003.2746, and arXiv:1007.2202 on the D1D5 system. We begin with some motivational material for black holes in string theory. In…

High Energy Physics - Theory · Physics 2010-12-02 Steven Avery

To model the process of absorption and emission of quanta by an extremal D1-D5 black hole in the dual CFT, we consider transitions between different Ramond vacua via absorption and emission of chiral primaries. We compute the probabilities…

High Energy Physics - Theory · Physics 2015-06-12 Oleg Lunin , Samir D. Mathur

It is generally agreed that black hole formation in gravity corresponds to thermalization in the dual CFT. It is sometimes argued that if the CFT evolution shows evidence of large redshift in gravity, then we have seen black hole formation…

High Energy Physics - Theory · Physics 2020-06-24 Shaun Hampton , Samir D. Mathur

The Higgs branch of the D1D5 system flows in the infrared to a two-dimensional N=(4,4) SCFT. This system is believed to have an "orbifold point" in its moduli space where the SCFT is a free sigma model with target space the symmetric…

High Energy Physics - Theory · Physics 2011-05-09 Steven G. Avery , Borun D. Chowdhury

We consider the D1D5 CFT near the orbifold point and develop methods for computing the mixing of untwisted operators to first order by using the OPE on the covering surface. We argue that the OPE on the cover encodes both the structure…

High Energy Physics - Theory · Physics 2017-08-02 Benjamin A. Burrington , Ian T. Jardine , Amanda W. Peet

We consider states of the D1-D5 CFT where only the left-moving sector is excited. As we deform away from the orbifold point, some of these states will remain BPS while others can `lift'. The lifting can be computed by a path integral…

High Energy Physics - Theory · Physics 2020-01-08 Bin Guo , Samir D. Mathur

We study correlation functions with fractional-mode excitations of the R-symmetry currents in D1-D5 CFT. We show how fractional-mode excitations lift to the covering surface associated with correlation functions as a specific sum of…

High Energy Physics - Theory · Physics 2026-02-11 V. A. Souza Alves , Andre Alves Lima , G. M. Sotkov , M. Stanishkov

The deformation operator of the D1D5 orbifold CFT, a twist 2 operator, drives the CFT towards the black hole dual and its physics is key to understanding thermalization in the D1D5 system. To further study this deformation, we extend…

High Energy Physics - Theory · Physics 2017-07-19 Zaq Carson , Ian T. Jardine , Amanda W. Peet

It is interesting to ask: how does the radial space direction emerge from the CFT in gauge-gravity duality? In this context we resolve a long-standing puzzle with the gravity duals of two classes of states in the D1D5 CFT. For each class…

High Energy Physics - Theory · Physics 2023-01-04 Bin Guo , Samir D. Mathur

The D1D5 CFT has a large set of states that are supersymmetric at the `free' orbifold point in moduli space. When we perturb away from this point, some of these states join into long multiplets and lift in energy, while others remain…

High Energy Physics - Theory · Physics 2020-04-22 Bin Guo , Samir D. Mathur
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