Chaos in CFT dual to rotating BTZ
Abstract We compute out-of-time-order correlators (OTOCs) in two-dimensional holographic conformal field theories (CFTs) with different left- and right-moving temperatures. Depending on whether the CFT lives on a spatial line or circle, the dual bulk geometry is a boosted BTZ black brane or a rotati...
Guardado en:
Autores principales: | , , |
---|---|
Formato: | article |
Lenguaje: | EN |
Publicado: |
SpringerOpen
2021
|
Materias: | |
Acceso en línea: | https://doaj.org/article/5c8f6156906148979f1cf92e184ca99e |
Etiquetas: |
Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
|
id |
oai:doaj.org-article:5c8f6156906148979f1cf92e184ca99e |
---|---|
record_format |
dspace |
spelling |
oai:doaj.org-article:5c8f6156906148979f1cf92e184ca99e2021-11-21T12:40:56ZChaos in CFT dual to rotating BTZ10.1007/JHEP11(2021)1051029-8479https://doaj.org/article/5c8f6156906148979f1cf92e184ca99e2021-11-01T00:00:00Zhttps://doi.org/10.1007/JHEP11(2021)105https://doaj.org/toc/1029-8479Abstract We compute out-of-time-order correlators (OTOCs) in two-dimensional holographic conformal field theories (CFTs) with different left- and right-moving temperatures. Depending on whether the CFT lives on a spatial line or circle, the dual bulk geometry is a boosted BTZ black brane or a rotating BTZ black hole. In the case when the spatial direction is non-compact, we generalise a computation of Roberts and Stanford and show that to reproduce the correct bulk answer a maximal channel contribution needs to be selected when using the identity block approximation. We use the correspondence between global conformal blocks and geodesic Witten diagrams to extend our results to CFTs on a spatial circle. In [1] it was shown that the OTOC for a rotating BTZ black hole exhibits a periodic modulation about an average exponential decay with Lyapunov exponent 2π/β. In the extremal limit where the black hole is maximally rotating, it was shown in [2] that the OTOC exhibits an average cubic growth, on which is superposed a sawtooth pattern which has small periods of Lyapunov growth due to the non-zero temperature of left-movers in the dual CFT. Our computations explain these results from a dual CFT perspective.Ben CrapsSurbhi KhetrapalCharles RabideauSpringerOpenarticleAdS-CFT CorrespondenceBlack Holes in String TheoryConformal Field TheoryNuclear and particle physics. Atomic energy. RadioactivityQC770-798ENJournal of High Energy Physics, Vol 2021, Iss 11, Pp 1-22 (2021) |
institution |
DOAJ |
collection |
DOAJ |
language |
EN |
topic |
AdS-CFT Correspondence Black Holes in String Theory Conformal Field Theory Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 |
spellingShingle |
AdS-CFT Correspondence Black Holes in String Theory Conformal Field Theory Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 Ben Craps Surbhi Khetrapal Charles Rabideau Chaos in CFT dual to rotating BTZ |
description |
Abstract We compute out-of-time-order correlators (OTOCs) in two-dimensional holographic conformal field theories (CFTs) with different left- and right-moving temperatures. Depending on whether the CFT lives on a spatial line or circle, the dual bulk geometry is a boosted BTZ black brane or a rotating BTZ black hole. In the case when the spatial direction is non-compact, we generalise a computation of Roberts and Stanford and show that to reproduce the correct bulk answer a maximal channel contribution needs to be selected when using the identity block approximation. We use the correspondence between global conformal blocks and geodesic Witten diagrams to extend our results to CFTs on a spatial circle. In [1] it was shown that the OTOC for a rotating BTZ black hole exhibits a periodic modulation about an average exponential decay with Lyapunov exponent 2π/β. In the extremal limit where the black hole is maximally rotating, it was shown in [2] that the OTOC exhibits an average cubic growth, on which is superposed a sawtooth pattern which has small periods of Lyapunov growth due to the non-zero temperature of left-movers in the dual CFT. Our computations explain these results from a dual CFT perspective. |
format |
article |
author |
Ben Craps Surbhi Khetrapal Charles Rabideau |
author_facet |
Ben Craps Surbhi Khetrapal Charles Rabideau |
author_sort |
Ben Craps |
title |
Chaos in CFT dual to rotating BTZ |
title_short |
Chaos in CFT dual to rotating BTZ |
title_full |
Chaos in CFT dual to rotating BTZ |
title_fullStr |
Chaos in CFT dual to rotating BTZ |
title_full_unstemmed |
Chaos in CFT dual to rotating BTZ |
title_sort |
chaos in cft dual to rotating btz |
publisher |
SpringerOpen |
publishDate |
2021 |
url |
https://doaj.org/article/5c8f6156906148979f1cf92e184ca99e |
work_keys_str_mv |
AT bencraps chaosincftdualtorotatingbtz AT surbhikhetrapal chaosincftdualtorotatingbtz AT charlesrabideau chaosincftdualtorotatingbtz |
_version_ |
1718418885233868800 |