Gravitational path integral from the T 2 deformation

Abstract We study a T 2 deformation of large N conformal field theories, a higher dimensional generalization of the T T ¯ $$ T\overline{T} $$ deformation. The deformed partition function satisfies a flow equation of the diffusion type. We solve this equation by finding its diffusion kernel, which is...

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Main Authors: Alexandre Belin, Aitor Lewkowycz, Gábor Sárosi
Format: Article
Language:English
Published: SpringerOpen 2020-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP09(2020)156
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author Alexandre Belin
Aitor Lewkowycz
Gábor Sárosi
author_facet Alexandre Belin
Aitor Lewkowycz
Gábor Sárosi
author_sort Alexandre Belin
collection DOAJ
description Abstract We study a T 2 deformation of large N conformal field theories, a higher dimensional generalization of the T T ¯ $$ T\overline{T} $$ deformation. The deformed partition function satisfies a flow equation of the diffusion type. We solve this equation by finding its diffusion kernel, which is given by the Euclidean gravitational path integral in d + 1 dimensions between two boundaries with Dirichlet boundary conditions for the metric. This is natural given the connection between the flow equation and the Wheeler-DeWitt equation, on which we offer a new perspective by giving a gauge-invariant relation between the deformed partition function and the radial WDW wave function. An interesting output of the flow equation is the gravitational path integral measure which is consistent with a constrained phase space quantization. Finally, we comment on the relation between the radial wave function and the Hartle-Hawking wave functions dual to states in the CFT, and propose a way of obtaining the volume of the maximal slice from the T 2 deformation.
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spelling doaj.art-4b561c68c6d84daa9df99b5507cc8bb92022-12-21T19:20:35ZengSpringerOpenJournal of High Energy Physics1029-84792020-09-012020913210.1007/JHEP09(2020)156Gravitational path integral from the T 2 deformationAlexandre Belin0Aitor Lewkowycz1Gábor Sárosi2CERN, Theory DivisionStanford Institute for Theoretical Physics, Department of Physics, Stanford UniversityCERN, Theory DivisionAbstract We study a T 2 deformation of large N conformal field theories, a higher dimensional generalization of the T T ¯ $$ T\overline{T} $$ deformation. The deformed partition function satisfies a flow equation of the diffusion type. We solve this equation by finding its diffusion kernel, which is given by the Euclidean gravitational path integral in d + 1 dimensions between two boundaries with Dirichlet boundary conditions for the metric. This is natural given the connection between the flow equation and the Wheeler-DeWitt equation, on which we offer a new perspective by giving a gauge-invariant relation between the deformed partition function and the radial WDW wave function. An interesting output of the flow equation is the gravitational path integral measure which is consistent with a constrained phase space quantization. Finally, we comment on the relation between the radial wave function and the Hartle-Hawking wave functions dual to states in the CFT, and propose a way of obtaining the volume of the maximal slice from the T 2 deformation.http://link.springer.com/article/10.1007/JHEP09(2020)156AdS-CFT CorrespondenceGauge-gravity correspondence
spellingShingle Alexandre Belin
Aitor Lewkowycz
Gábor Sárosi
Gravitational path integral from the T 2 deformation
Journal of High Energy Physics
AdS-CFT Correspondence
Gauge-gravity correspondence
title Gravitational path integral from the T 2 deformation
title_full Gravitational path integral from the T 2 deformation
title_fullStr Gravitational path integral from the T 2 deformation
title_full_unstemmed Gravitational path integral from the T 2 deformation
title_short Gravitational path integral from the T 2 deformation
title_sort gravitational path integral from the t 2 deformation
topic AdS-CFT Correspondence
Gauge-gravity correspondence
url http://link.springer.com/article/10.1007/JHEP09(2020)156
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