Baby universe operators in the ETH matrix model of double-scaled SYK

Abstract We consider the baby universe operator B a $$ {\mathcal{B}}_a $$ in the double-scaled SYK (DSSYK) model, which creates a baby universe of size a. We find that B a $$ {\mathcal{B}}_a $$ is written in terms of the transfer matrix T, and vice versa. In particular, the identity operator on the...

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Main Author: Kazumi Okuyama
Format: Article
Language:English
Published: SpringerOpen 2024-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP10(2024)249
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author Kazumi Okuyama
author_facet Kazumi Okuyama
author_sort Kazumi Okuyama
collection DOAJ
description Abstract We consider the baby universe operator B a $$ {\mathcal{B}}_a $$ in the double-scaled SYK (DSSYK) model, which creates a baby universe of size a. We find that B a $$ {\mathcal{B}}_a $$ is written in terms of the transfer matrix T, and vice versa. In particular, the identity operator on the chord Hilbert space is expanded as a linear combination of B a $$ {\mathcal{B}}_a $$ , which implies that the disk partition function of DSSYK is written as a linear combination of trumpets. We also find that the thermofield double state of DSSYK is generated by a pair of baby universe operators, which corresponds to a double trumpet. This can be thought of as a concrete realization of the idea of ER=EPR.
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institution Kabale University
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publishDate 2024-10-01
publisher SpringerOpen
record_format Article
series Journal of High Energy Physics
spelling doaj-art-b34b070d810a4ea6bde0d19dbf8a1c992024-12-08T12:12:48ZengSpringerOpenJournal of High Energy Physics1029-84792024-10-0120241011410.1007/JHEP10(2024)249Baby universe operators in the ETH matrix model of double-scaled SYKKazumi Okuyama0Department of Physics, Shinshu UniversityAbstract We consider the baby universe operator B a $$ {\mathcal{B}}_a $$ in the double-scaled SYK (DSSYK) model, which creates a baby universe of size a. We find that B a $$ {\mathcal{B}}_a $$ is written in terms of the transfer matrix T, and vice versa. In particular, the identity operator on the chord Hilbert space is expanded as a linear combination of B a $$ {\mathcal{B}}_a $$ , which implies that the disk partition function of DSSYK is written as a linear combination of trumpets. We also find that the thermofield double state of DSSYK is generated by a pair of baby universe operators, which corresponds to a double trumpet. This can be thought of as a concrete realization of the idea of ER=EPR.https://doi.org/10.1007/JHEP10(2024)249AdS-CFT Correspondence2D GravityRandom Systems
spellingShingle Kazumi Okuyama
Baby universe operators in the ETH matrix model of double-scaled SYK
Journal of High Energy Physics
AdS-CFT Correspondence
2D Gravity
Random Systems
title Baby universe operators in the ETH matrix model of double-scaled SYK
title_full Baby universe operators in the ETH matrix model of double-scaled SYK
title_fullStr Baby universe operators in the ETH matrix model of double-scaled SYK
title_full_unstemmed Baby universe operators in the ETH matrix model of double-scaled SYK
title_short Baby universe operators in the ETH matrix model of double-scaled SYK
title_sort baby universe operators in the eth matrix model of double scaled syk
topic AdS-CFT Correspondence
2D Gravity
Random Systems
url https://doi.org/10.1007/JHEP10(2024)249
work_keys_str_mv AT kazumiokuyama babyuniverseoperatorsintheethmatrixmodelofdoublescaledsyk