G. Larios

activity

20192025

most citedThe spectrum of marginally-deformed

N = 2

CFTs with AdS

_{4}

S-fold duals of type IIB

21 citations · 119 across the 10 of their papers we have counts for

collaborators

Showing hep-thShow all

11 papers · 1 filter

hep-th2025

Machine Learning the Conformal Manifold of Holographic CFT $_{2}$ s

Bastien Duboeuf, Camille Eloy, Gabriel Larios

We investigate the structure of conformal manifolds around AdS $_{3} \times S^{3}$ which lift from continuous flat directions in the scalar potential of gauged supergravity resulting fr…

hep-th2024★ 6 cited

Charting the Conformal Manifold of Holographic CFT $_{2}$ 's

Camille Eloy, Gabriel Larios

We construct new continuous families of $AdS_{3} \times S^{3} \times T^{4}$ and $AdS_{3} \times S^{3} \times S^{3} \times S^{1}$ solutions in heterotic and type II supergravities. T…

hep-th2023

Singular limits in STU supergravity

Gabriel Larios, Christopher N. Pope, Haoyu Zhang

We analyse the STU sectors of the four-dimensional maximal gauged supergravities with gauge groups $SO (8)$ , $SO (6) ⋉ R^{12}$ and $[{\rm SO(6)}\times{\rm SO…

hep-th2023

On non-supersymmetric stable marginal deformations in AdS $_{3}$ /CFT $_{2}$

Camille Eloy, Gabriel Larios

We discuss a continuous family of non-supersymmetric AdS $_{3} \times S^{3} \times T^{4}$ vacua in heterotic and type II supergravities whose complete Kaluza-Klein spectrum is computed…

hep-th2021★ 17 cited

Triality and the consistent reductions on $AdS_{3} \times S^{3}$

Camille Eloy, Gabriel Larios, Henning Samtleben

We study compactifications on $AdS_{3} \times S^{3}$ and deformations thereof. We exploit the triality symmetry of the underlying duality group $SO (4, 4)$ of three-dimensiona…

hep-th2021★ 21 cited

The spectrum of marginally-deformed $N = 2$ CFTs with AdS $_{4}$ S-fold duals of type IIB

Mattia Cesàro, Gabriel Larios, Oscar Varela

A holographic duality was recently established between an $N = 4$ non-geometric AdS $_{4}$ solution of type IIB supergravity in the so-called S-fold class, and a three-dimension…

hep-th2021★ 16 cited

Supersymmetric spectroscopy on AdS $_{4} \times S^{7}$ and AdS $_{4} \times S^{6}$

Mattia Cesaro, Gabriel Larios, Oscar Varela

New techniques based on Exceptional Field Theory have recently allowed for the calculation of the Kaluza-Klein spectra of certain AdS $_{4}$ solutions of $D = 11$ and massive IIA superg…

hep-th2020★ 11 cited

A Cubic Deformation of ABJM: The Squashed, Stretched, Warped, and Perturbed Gets Invaded

Mattia Cesaro, Gabriel Larios, Oscar Varela

A superpotential deformation that is cubic in one of the chiral superfields of ABJM makes the latter theory flow into a new, $N = 2$ superconformal phase. This is holographica…

hep-th2019★ 14 cited

Universal properties of Kaluza-Klein gravitons

Kevin Dimmitt, Gabriel Larios, Praxitelis Ntokos +1

Vacua of different gaugings of $D = 4$ $N = 8$ supergravity that preserve the same supersymmetries and bosonic symmetry tend to exhibit the same universal mass spectrum within t…

hep-th2019★ 15 cited

Minimal $D = 4$ $N = 2$ supergravity from $D = 11$ : An M-theory free lunch

Gabriel Larios, Oscar Varela

We present a new consistent truncation of $D = 11$ supergravity to $D = 4$ $N = 2$ minimal gauged supergravity, on the seven-dimensional internal Riemannian space corresponding…

hep-th2019★ 19 cited

Embedding the SU(3) sector of SO(8) supergravity in $D = 11$

Gabriel Larios, Praxitelis Ntokos, Oscar Varela

The SU(3)--invariant sector of maximal supergravity in four dimensions with an SO(8) gauging is uplifted to $D = 11$ supergravity. In order to do this, the SU(3)--neutral sector of t…

Machine Learning the Conformal Manifold of Holographic CFT2​s

Charting the Conformal Manifold of Holographic CFT2​'s

Singular limits in STU supergravity

On non-supersymmetric stable marginal deformations in AdS3​/CFT2​

Triality and the consistent reductions on AdS3​×S3

The spectrum of marginally-deformed N=2 CFTs with AdS4​ S-fold duals of type IIB

Supersymmetric spectroscopy on AdS4​×S7 and AdS4​×S6