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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Janus solutions in three-dimensional N $$ \mathcalN} $$ = 8 gauged supergravity ; volume:2021 ; number:5 ; day:3 ; month:5 ; year:2021 ; pages:1-19 ; date:5.2021
Journal of high energy physics ; 2021, Heft 5 (3.5.2021), 1-19, 5.2021

Creator: Chen, Kevin
Gutperle, Michael

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2021)008

URN: urn:nbn:de:101:1-2021111520120713010020

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

Last update: 15.08.2025, 7:22 AM CEST

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Chen, Kevin
Gutperle, Michael
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

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

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

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

Supersymmetric solitons in gauged 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

$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

$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

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

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

Janus solutions in six-dimensional gauged supergravity

$The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity$

The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity

$Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions$

Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions

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

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

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

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

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

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

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

Supersymmetric solitons in gauged 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

$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

$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

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

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

Janus solutions in six-dimensional gauged supergravity

$The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity$

The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity

$Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions$

Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions

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

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

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

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

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

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

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

Supersymmetric solitons in gauged 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

$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

$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

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

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

Janus solutions in six-dimensional gauged supergravity

$The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity$

The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity

$Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions$

Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions

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

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Other Objects (12)

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

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

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

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

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

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

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

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

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

Janus solutions in six-dimensional gauged supergravity

The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity

Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions

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

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

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

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

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

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

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

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

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

Janus solutions in six-dimensional gauged supergravity

The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity

Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions

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

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

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

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

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

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

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

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

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

Janus solutions in six-dimensional gauged supergravity

The attractor flow for AdS5 black holes in N $$ \mathcalN} $$ = 2 gauged supergravity

Magnetically-charged supersymmetric flows of gauged N=8 $$ \mathcalN}=8 $$ supergravity in five dimensions

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