N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

Umfang: Online-Ressource, 1 online resource.

Sprache: Englisch

Erschienen in: N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity ; volume:2023 ; number:6 ; day:13 ; month:6 ; year:2023 ; pages:1-39 ; date:6.2023
Journal of high energy physics ; 2023, Heft 6 (13.6.2023), 1-39, 6.2023

Urheber: Chamorro-Burgos, Miguel
Guarino, Adolfo
Sterckx, Colin

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2023)068

URN: urn:nbn:de:101:1-2023092112504594003528

Rechteinformation: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Letzte Aktualisierung: 14.08.2025, 10:48 MESZ

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Beteiligte

Chamorro-Burgos, Miguel
Guarino, Adolfo
Sterckx, Colin
SpringerLink (Online service)

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Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity$

Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

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Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

$Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons$

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

$Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory$

N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity$

Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

$Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity$

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

$Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons$

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

$Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory$

N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity$

Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity

$New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity$

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

$Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity$

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

$Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons$

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

$Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory$

N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

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Ähnliche Objekte (12)

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity

New non-extremal and BPS hairy black holes in gauged N $$ \mathcalN} $$ = 2 and N $$ \mathcalN} $$ = 8 supergravity

Nernst branes with Lifshitz asymptotics in N $$ \mathcalN} $$ = 2 gauged supergravity

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

Supersymmetric Janus solutions of dyonic ISO(7)-gauged N $$ \mathcalN} $$ = 8 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ =2 supersymmetric Janus solutions and flows: from gauged supergravity to M theory

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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