A bound on chaos from stability
Abstract We explore the quantum chaos of the coadjoint orbit action of diffeomorphism group of S 1. We study quantum fluctuation around a saddle point to evaluate the soft mode contribution to the out-of-time-ordered correlator. We show that the stability condition of the semi-classical analysis of...
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2021
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oai:doaj.org-article:a6a0f4fc31ad4e4e8125a8aee7ffd73d2021-11-14T12:40:21ZA bound on chaos from stability10.1007/JHEP11(2021)0971029-8479https://doaj.org/article/a6a0f4fc31ad4e4e8125a8aee7ffd73d2021-11-01T00:00:00Zhttps://doi.org/10.1007/JHEP11(2021)097https://doaj.org/toc/1029-8479Abstract We explore the quantum chaos of the coadjoint orbit action of diffeomorphism group of S 1. We study quantum fluctuation around a saddle point to evaluate the soft mode contribution to the out-of-time-ordered correlator. We show that the stability condition of the semi-classical analysis of the coadjoint orbit found in [1] leads to the upper bound on the Lyapunov exponent which is identical to the bound on chaos proven in [2]. The bound is saturated by the coadjoint orbit Diff(S 1)/SL(2) while the other stable orbit Diff(S 1)/U(1) where the SL(2, ℝ) is broken to U(1) has non-maximal Lyapunov exponent.Junggi YoonSpringerOpenarticle2D GravityAdS-CFT CorrespondenceField Theories in Lower DimensionsNuclear and particle physics. Atomic energy. RadioactivityQC770-798ENJournal of High Energy Physics, Vol 2021, Iss 11, Pp 1-14 (2021) |
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2D Gravity AdS-CFT Correspondence Field Theories in Lower Dimensions Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 |
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2D Gravity AdS-CFT Correspondence Field Theories in Lower Dimensions Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 Junggi Yoon A bound on chaos from stability |
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Abstract We explore the quantum chaos of the coadjoint orbit action of diffeomorphism group of S 1. We study quantum fluctuation around a saddle point to evaluate the soft mode contribution to the out-of-time-ordered correlator. We show that the stability condition of the semi-classical analysis of the coadjoint orbit found in [1] leads to the upper bound on the Lyapunov exponent which is identical to the bound on chaos proven in [2]. The bound is saturated by the coadjoint orbit Diff(S 1)/SL(2) while the other stable orbit Diff(S 1)/U(1) where the SL(2, ℝ) is broken to U(1) has non-maximal Lyapunov exponent. |
format |
article |
author |
Junggi Yoon |
author_facet |
Junggi Yoon |
author_sort |
Junggi Yoon |
title |
A bound on chaos from stability |
title_short |
A bound on chaos from stability |
title_full |
A bound on chaos from stability |
title_fullStr |
A bound on chaos from stability |
title_full_unstemmed |
A bound on chaos from stability |
title_sort |
bound on chaos from stability |
publisher |
SpringerOpen |
publishDate |
2021 |
url |
https://doaj.org/article/a6a0f4fc31ad4e4e8125a8aee7ffd73d |
work_keys_str_mv |
AT junggiyoon aboundonchaosfromstability AT junggiyoon boundonchaosfromstability |
_version_ |
1718429123256254464 |