$$ \mathcal{N} $$ = (4, 4) supersymmetric AdS3 solutions in d = 11

A bstract We derive necessary and sufficient conditions for AdS 3 solutions of d = 11 supergravity to preserve $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (1, 1) supersymmetry in terms of G-structures. Such solutions necessarily support an SU(3)-structure on the internal 8-manifold M 8 , in terms of which we phrase the conditions for supersymmetry preservation. We use this to derive the local form of all $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (4, 4) supersymmetric AdS 3 solutions in d = 11, for which M 8 decomposes as a foliation of a 3-sphere over a 5 dimensional base. There are 3 independent classes, 2 of which preserve the small superconformal algebra and one preserving its large counterpart for which M 5 contains a second 3-sphere. We show that for each solution with large (4, 4) supersymmetry there are two corresponding solutions with small (4, 4), one for which M 5 maintains its 3-sphere, one where this blows up to ℝ 3 which can be compactified to 𝕋 3 . We use our results to construct several new solutions that lie within our derived classes as well as recovering some existing solutions.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-05-20
DOI
https://doi.org/10.1007/jhep05(2025)163
Citations
1
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
1.87

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article

$$ \mathcal{N} $$ = (4, 4) supersymmetric AdS3 solutions in d = 11

A. Conti, Niall T. Macpherson
1 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
1.87
article

$$ \mathcal{N} $$ = (4, 4) supersymmetric AdS3 solutions in d = 11

A. Conti, Niall T. Macpherson
article en
1 citations

Abstract

A bstract We derive necessary and sufficient conditions for AdS 3 solutions of d = 11 supergravity to preserve $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (1, 1) supersymmetry in terms of G-structures. Such solutions necessarily support an SU(3)-structure on the internal 8-manifold M 8 , in terms of which we phrase the conditions for supersymmetry preservation. We use this to derive the local form of all $$ \mathcal{N} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>N</mml:mi> </mml:math> = (4, 4) supersymmetric AdS 3 solutions in d = 11, for which M 8 decomposes as a foliation of a 3-sphere over a 5 dimensional base. There are 3 independent classes, 2 of which preserve the small superconformal algebra and one preserving its large counterpart for which M 5 contains a second 3-sphere. We show that for each solution with large (4, 4) supersymmetry there are two corresponding solutions with small (4, 4), one for which M 5 maintains its 3-sphere, one where this blows up to ℝ 3 which can be compactified to 𝕋 3 . We use our results to construct several new solutions that lie within our derived classes as well as recovering some existing solutions.

Journal of High Energy PhysicsVol. 2025(5)
Universidad de Oviedo (ES)
Ministerio de Ciencia, Innovación y Universidades
Openalex Percentile: Top 14%
Black Holes and Theoretical Physics
1.87
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