A note on background independence in AdS3 string theory

Abstract In this note, we comment on the path integral formulation of string theory on M $$ \mathcal{M} $$ × S3 × T 4 $$ {\mathbbm{T}}^4 $$ where M $$ \mathcal{M} $$ is any hyperbolic 3-manifold. In the special case of k = 1 units of NS-NS flux, we provide a covariant description of the worldsheet t...

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Main Author: Bob Knighton
Format: Article
Language:English
Published: SpringerOpen 2025-02-01
Series:Journal of High Energy Physics
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Online Access:https://doi.org/10.1007/JHEP02(2025)004
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author Bob Knighton
author_facet Bob Knighton
author_sort Bob Knighton
collection DOAJ
description Abstract In this note, we comment on the path integral formulation of string theory on M $$ \mathcal{M} $$ × S3 × T 4 $$ {\mathbbm{T}}^4 $$ where M $$ \mathcal{M} $$ is any hyperbolic 3-manifold. In the special case of k = 1 units of NS-NS flux, we provide a covariant description of the worldsheet theory and argue that the path integral depends only on the details of the conformal boundary ∂ M $$ \partial \mathcal{M} $$ , making the background independence of this theory manifest. We provide a simple path integral argument that the path integral localizes onto holomorphic covering maps from the worldsheet to the boundary. For closed manifolds M $$ \mathcal{M} $$ , the gravitational path integral is argued to be trivial. Finally, we comment on the effect of continuous deformations of the worldsheet theory which introduce non-minimal string tension.
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spelling doaj-art-21e7e6b564c94de6a08241f5040afc602025-02-09T12:08:54ZengSpringerOpenJournal of High Energy Physics1029-84792025-02-012025211710.1007/JHEP02(2025)004A note on background independence in AdS3 string theoryBob Knighton0Department of Applied Mathematics & Theoretical Physics, University of CambridgeAbstract In this note, we comment on the path integral formulation of string theory on M $$ \mathcal{M} $$ × S3 × T 4 $$ {\mathbbm{T}}^4 $$ where M $$ \mathcal{M} $$ is any hyperbolic 3-manifold. In the special case of k = 1 units of NS-NS flux, we provide a covariant description of the worldsheet theory and argue that the path integral depends only on the details of the conformal boundary ∂ M $$ \partial \mathcal{M} $$ , making the background independence of this theory manifest. We provide a simple path integral argument that the path integral localizes onto holomorphic covering maps from the worldsheet to the boundary. For closed manifolds M $$ \mathcal{M} $$ , the gravitational path integral is argued to be trivial. Finally, we comment on the effect of continuous deformations of the worldsheet theory which introduce non-minimal string tension.https://doi.org/10.1007/JHEP02(2025)004AdS-CFT CorrespondenceConformal Field Models in String Theory
spellingShingle Bob Knighton
A note on background independence in AdS3 string theory
Journal of High Energy Physics
AdS-CFT Correspondence
Conformal Field Models in String Theory
title A note on background independence in AdS3 string theory
title_full A note on background independence in AdS3 string theory
title_fullStr A note on background independence in AdS3 string theory
title_full_unstemmed A note on background independence in AdS3 string theory
title_short A note on background independence in AdS3 string theory
title_sort note on background independence in ads3 string theory
topic AdS-CFT Correspondence
Conformal Field Models in String Theory
url https://doi.org/10.1007/JHEP02(2025)004
work_keys_str_mv AT bobknighton anoteonbackgroundindependenceinads3stringtheory
AT bobknighton noteonbackgroundindependenceinads3stringtheory