Spectrum of end of the world branes in holographic BCFTs
Abstract We study overlaps between two regularized boundary states in conformal field theories. Regularized boundary states are dual to end of the world branes in an AdS black hole via the AdS/BCFT. Thus they can be regarded as microstates of a single sided black hole. Owing to the open-closed duali...
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doaj-c03264c2afc24b5fbe69c34685d0d4c22021-06-06T11:08:24ZengSpringerOpenJournal of High Energy Physics1029-84792021-06-012021611910.1007/JHEP06(2021)023Spectrum of end of the world branes in holographic BCFTsMasamichi Miyaji0Tadashi Takayanagi1Tomonori Ugajin2Berkeley Center for Theoretical Physics, Department of Physics, University of CaliforniaCenter for Gravitational Physics, Yukawa Institute for Theoretical Physics, Kyoto UniversityCenter for Gravitational Physics, Yukawa Institute for Theoretical Physics, Kyoto UniversityAbstract We study overlaps between two regularized boundary states in conformal field theories. Regularized boundary states are dual to end of the world branes in an AdS black hole via the AdS/BCFT. Thus they can be regarded as microstates of a single sided black hole. Owing to the open-closed duality, such an overlap between two different regularized boundary states is exponentially suppressed as ψ a ψ b ∼ e − O h ab min $$ \left\langle \left.{\psi}_a\right|{\psi}_b\right\rangle \sim {e}^{-O\left({h}_{ab}^{\left(\min \right)}\right)} $$ , where h ab min $$ {h}_{ab}^{\left(\min \right)} $$ is the lowest energy of open strings which connect two different boundaries a and b. Our gravity dual analysis leads to h ab min $$ {h}_{ab}^{\left(\min \right)} $$ = c/24 for a pure AdS3 gravity. This shows that a holographic boundary state is a random vector among all left-right symmetric states, whose number is given by a square root of the number of all black hole microstates. We also perform a similar computation in higher dimensions, and find that h ab min $$ {h}_{ab}^{\left(\min \right)} $$ depends on the tensions of the branes. In our analysis of holographic boundary states, the off diagonal elements of the inner products can be computed directly from on-shell gravity actions, as opposed to earlier calculations of inner products of microstates in two dimensional gravity.https://doi.org/10.1007/JHEP06(2021)023AdS-CFT CorrespondenceBoundary Quantum Field TheoryConformal Field Theory |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Masamichi Miyaji Tadashi Takayanagi Tomonori Ugajin |
spellingShingle |
Masamichi Miyaji Tadashi Takayanagi Tomonori Ugajin Spectrum of end of the world branes in holographic BCFTs Journal of High Energy Physics AdS-CFT Correspondence Boundary Quantum Field Theory Conformal Field Theory |
author_facet |
Masamichi Miyaji Tadashi Takayanagi Tomonori Ugajin |
author_sort |
Masamichi Miyaji |
title |
Spectrum of end of the world branes in holographic BCFTs |
title_short |
Spectrum of end of the world branes in holographic BCFTs |
title_full |
Spectrum of end of the world branes in holographic BCFTs |
title_fullStr |
Spectrum of end of the world branes in holographic BCFTs |
title_full_unstemmed |
Spectrum of end of the world branes in holographic BCFTs |
title_sort |
spectrum of end of the world branes in holographic bcfts |
publisher |
SpringerOpen |
series |
Journal of High Energy Physics |
issn |
1029-8479 |
publishDate |
2021-06-01 |
description |
Abstract We study overlaps between two regularized boundary states in conformal field theories. Regularized boundary states are dual to end of the world branes in an AdS black hole via the AdS/BCFT. Thus they can be regarded as microstates of a single sided black hole. Owing to the open-closed duality, such an overlap between two different regularized boundary states is exponentially suppressed as ψ a ψ b ∼ e − O h ab min $$ \left\langle \left.{\psi}_a\right|{\psi}_b\right\rangle \sim {e}^{-O\left({h}_{ab}^{\left(\min \right)}\right)} $$ , where h ab min $$ {h}_{ab}^{\left(\min \right)} $$ is the lowest energy of open strings which connect two different boundaries a and b. Our gravity dual analysis leads to h ab min $$ {h}_{ab}^{\left(\min \right)} $$ = c/24 for a pure AdS3 gravity. This shows that a holographic boundary state is a random vector among all left-right symmetric states, whose number is given by a square root of the number of all black hole microstates. We also perform a similar computation in higher dimensions, and find that h ab min $$ {h}_{ab}^{\left(\min \right)} $$ depends on the tensions of the branes. In our analysis of holographic boundary states, the off diagonal elements of the inner products can be computed directly from on-shell gravity actions, as opposed to earlier calculations of inner products of microstates in two dimensional gravity. |
topic |
AdS-CFT Correspondence Boundary Quantum Field Theory Conformal Field Theory |
url |
https://doi.org/10.1007/JHEP06(2021)023 |
work_keys_str_mv |
AT masamichimiyaji spectrumofendoftheworldbranesinholographicbcfts AT tadashitakayanagi spectrumofendoftheworldbranesinholographicbcfts AT tomonoriugajin spectrumofendoftheworldbranesinholographicbcfts |
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