The higher-dimensional origin of five-dimensional $$ \mathcal{N} $$ = 2 gauged supergravities

Josse, Grégoire; Malek, Emanuel; Petrini, Michela; Waldram, Daniel

doi:10.1007/jhep06(2022)003

Cited by 6 publications

(3 citation statements)

References 67 publications

(195 reference statements)

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“…The eigenvalues of M (vector)P M will correspond to the vector squared-mass spectrum 5 . Let us observe that det…”

Section: Vector Mass Matrixmentioning

confidence: 99%

“…As far as the construction of consistent truncations within maximal lower-dimensional supergravities is concerned, Exceptional Field Theory [1,2] provides an efficient framework for embedding certain lower dimensional models into superstring or M-theories and for studying perturbative stability of their solutions [3]. In the more general case important progress has been made towards a systematic construction of lower-dimensional consistent truncations [4,5]. In this case the set-up is the one of Generalised Geometry in which a wide class of consistent truncations can be described by exploiting the concept of generalised G S -structure manifolds with singlet intrinsic torsion.…”

Section: Introductionmentioning

confidence: 99%

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Gauged $\mathcal{N}=3,D=4$ Supergravity: a new web of marginally connected vacua

Fré,

Giambrone,

Ruggeri

et al. 2022

Preprint

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We analyze the vacuum structure of N = 3, D = 4 supergravity coupled to 9 vector multiplets with gauge group SO(3) × SU(3). Aside from the central N = 3 AdS 4 vacuum at the origin, on which the supermultiplet structure reproduces the massless sector of M-theory compactified on N 0,1,0 , we find a rich structure of AdS 4 vacua preserving N = 0, 1, 2, 3 supersymmetry. These new vacua are arranged in a manifold spanned by scalar fields corresponding to exactly marginal deformations of the dual CFT. This manifold has the form T 3 /K, where K is a discrete subgroup of the gauge group: N = 3, 2 and 1 vacua correspond, respectively, to a point, a line and a surface in the three-dimensional vacuum manifold. We study RG flows from the central N = 3 vacuum and elaborate on the possible higher dimensional origin of the new vacua. For the reader's convenience we also provide a review of the embedding tensor formulation of D = 4, N = 3 gauged supergravities. In particular we provide formulas involving the fermion shift tensors and mass matrices in N = 3 theories, which can be applied to a generic gauging.

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“…The eigenvalues of M (vector)P M will correspond to the vector squared-mass spectrum 5 . Let us observe that det…”

Section: Vector Mass Matrixmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Gauged $\mathcal{N}=3,D=4$ Supergravity: a new web of marginally connected vacua

Fré,

Giambrone,

Ruggeri

et al. 2022

Preprint

View full text Add to dashboard Cite

show abstract

“…Examples include consistent truncations on spheres down to maximal gauged supergravities [1][2][3][4][5][6][7], Sasaki-Einstein manifolds [8][9][10][11], weak-G 2 holonomy manifolds [8] and tri-Sasakian manifolds [12], SU(2)-structure [13,14] and SU(3)-structure [15] manifolds, as well as spaces including brane singularities [16]. Recently, a framework based on exceptional generalised geometry and exceptional field theory has emerged, that allows for a systematic treatment of consistent truncations [17][18][19][20][21]. Despite these successes the exceptional field theory framework for consistent truncations has only been fully worked out for reductions to maximal and half-maximal gauged supergravities.…”

Section: Introductionmentioning

confidence: 99%

A plethora of Type IIA embeddings for d = 5 minimal supergravity

Couzens

Macpherson

Passias

2023

J. High Energ. Phys.

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We construct multiple embeddings of all solutions of d = 5 minimal (un)gauged supergravity into massive Type IIA supergravity. The internal spaces and warpings of such embeddings are the same as those of the $$ \mathcal{N} $$ N = 1 supersymmetric (Mink5) AdS5 vacua, with the slight modification that the U(1) R-symmetry direction becomes fibered over the external space by the d = 5 gauge field. In addition the fluxes are appropriately modified. There are many distinct types of the aforementioned internal spaces and as such many different embeddings of the d = 5 supergravity. As examples of our setup we provide new solutions dual to six-dimensional, $$ \mathcal{N} $$ N = (1, 0) SCFTs compactified on the product of a constant curvature Riemann surface and a spindle. We also provide a multitude of massive Type IIA embeddings for rotating, asymptotically AdS5 black hole solutions.

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Wrapped M5-branes and AdS5 black holes

Bobev

Dimitrov

Vekemans

2023

J. High Energ. Phys.

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We use consistent truncations in supergravity to show that the backreaction of N rotating M5-branes wrapped on a Riemann surface leads to asymptotically AdS5 black hole solutions of 11d supergravity. We discuss the thermodynamic properties of these black holes focusing on their supersymmetric limit. The Bekenstein-Hawking entropy of the supersymmetric black holes scales as N3 and can be reproduced by the superconformal index of the holographically dual 4d $$ \mathcal{N} $$ N = 1 SCFTs of class $$ \mathcal{S} $$ S .

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The higher-dimensional origin of five-dimensional $$ \mathcal{N} $$ = 2 gauged supergravities

Cited by 6 publications

References 67 publications

Gauged $\mathcal{N}=3,D=4$ Supergravity: a new web of marginally connected vacua

Gauged $\mathcal{N}=3,D=4$ Supergravity: a new web of marginally connected vacua

A plethora of Type IIA embeddings for d = 5 minimal supergravity

Wrapped M5-branes and AdS5 black holes

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