Toric gravitational instantons in gauged supergravity

<p>We introduce a general class of toric gravitational instantons in <em>D</em> = 4, <em>N</em> = 2 gauged supergravity, namely Euclidean supersymmetric solutions with <em>U</em>(1)<sup>2</sup> isometry. Such solutions are specified by a “supergr...

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Main Authors: Benetti Genolini, P, Gauntlett, JP, Jiao, Y, Lüscher, A, Sparks, J
Format: Journal article
Language:English
Published: American Physical Society 2025
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author Benetti Genolini, P
Gauntlett, JP
Jiao, Y
Lüscher, A
Sparks, J
author_facet Benetti Genolini, P
Gauntlett, JP
Jiao, Y
Lüscher, A
Sparks, J
author_sort Benetti Genolini, P
collection OXFORD
description <p>We introduce a general class of toric gravitational instantons in <em>D</em> = 4, <em>N</em> = 2 gauged supergravity, namely Euclidean supersymmetric solutions with <em>U</em>(1)<sup>2</sup> isometry. Such solutions are specified by a “supergravity labelled polytope”, where the labels encode the 4-manifold topology, the choice of magnetic fluxes, and certain signs associated to the Killing spinor. Equivariant localization allows us to write down the gravitational free energy for such a solution, assuming it exists, and study its properties. These results open the way for a systematic study of holography in this setting, where the dual large N field theories are defined on the boundary 3-manifolds, which are (squashed) lens spaces <em>L</em>(<em>p</em>, <em>q</em>) or generalizations with orbifold singularities.</p>
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spelling oxford-uuid:30814949-45c3-4087-ba72-76c371dbd1632025-02-07T11:39:20ZToric gravitational instantons in gauged supergravityJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:30814949-45c3-4087-ba72-76c371dbd163EnglishSymplectic ElementsAmerican Physical Society2025Benetti Genolini, PGauntlett, JPJiao, YLüscher, ASparks, J<p>We introduce a general class of toric gravitational instantons in <em>D</em> = 4, <em>N</em> = 2 gauged supergravity, namely Euclidean supersymmetric solutions with <em>U</em>(1)<sup>2</sup> isometry. Such solutions are specified by a “supergravity labelled polytope”, where the labels encode the 4-manifold topology, the choice of magnetic fluxes, and certain signs associated to the Killing spinor. Equivariant localization allows us to write down the gravitational free energy for such a solution, assuming it exists, and study its properties. These results open the way for a systematic study of holography in this setting, where the dual large N field theories are defined on the boundary 3-manifolds, which are (squashed) lens spaces <em>L</em>(<em>p</em>, <em>q</em>) or generalizations with orbifold singularities.</p>
spellingShingle Benetti Genolini, P
Gauntlett, JP
Jiao, Y
Lüscher, A
Sparks, J
Toric gravitational instantons in gauged supergravity
title Toric gravitational instantons in gauged supergravity
title_full Toric gravitational instantons in gauged supergravity
title_fullStr Toric gravitational instantons in gauged supergravity
title_full_unstemmed Toric gravitational instantons in gauged supergravity
title_short Toric gravitational instantons in gauged supergravity
title_sort toric gravitational instantons in gauged supergravity
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AT gauntlettjp toricgravitationalinstantonsingaugedsupergravity
AT jiaoy toricgravitationalinstantonsingaugedsupergravity
AT luschera toricgravitationalinstantonsingaugedsupergravity
AT sparksj toricgravitationalinstantonsingaugedsupergravity