Asymptotically free AdS3/CFT2

A bstract We propose a new AdS 3 /CFT 2 duality, in which the bulk string theory has a target spacetime AdS 3 times a squashed three-sphere S ♭ 3 , and the dual CFT 2 is a symmetric product of sigma models on ℝ ϕ × S ♭ 3 , deformed by a ϕ -dependent ℤ 2 twist operator. The duality maps the asymptoti...

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Veröffentlicht in:The journal of high energy physics Jg. 2022; H. 1; S. 1 - 106
Hauptverfasser: Balthazar, Bruno, Giveon, Amit, Kutasov, David, Martinec, Emil J.
Format: Journal Article
Sprache:Englisch
Veröffentlicht: Berlin/Heidelberg Springer Berlin Heidelberg 01.01.2022
Springer Nature B.V
Springer Nature
SpringerOpen
Schlagworte:
AdS-CFT Correspondence
Asymptotic properties
Classical and Quantum Gravitation
Conformal Field Models in String Theory
Elementary Particles
Flux density
High energy physics
Long strings
Physics
Physics and Astronomy
PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
Quantum Field Theories
Quantum Field Theory
Quantum Physics
Regular Article - Theoretical Physics
Relativity Theory
String Theory
Long strings
AdS-CFT Correspondence
Conformal Field Models in String Theory
ISSN:1029-8479, 1029-8479
Online-Zugang:Volltext
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Zusammenfassung:A bstract We propose a new AdS 3 /CFT 2 duality, in which the bulk string theory has a target spacetime AdS 3 times a squashed three-sphere S ♭ 3 , and the dual CFT 2 is a symmetric product of sigma models on ℝ ϕ × S ♭ 3 , deformed by a ϕ -dependent ℤ 2 twist operator. The duality maps the asymptotic region of AdS 3 to the region ϕ → ∞ , where the twist interaction in the CFT 2 turns off. The AdS 3 backgrounds in question have R AdS < ℓ s , and so lie on the string side of the string/black hole correspondence transition. As a consequence, the high energy density of states consists of a string gas in AdS 3 rather than an ensemble of BTZ black holes. This property allows us to derive the dual CFT 2 by a systematic analysis of the worldsheet string theory on AdS 3 .
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USDOE Office of Science (SC), High Energy Physics (HEP)
SC0009924
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP01(2022)008