New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity ; volume:2022 ; number:3 ; day:16 ; month:3 ; year:2022 ; pages:1-30 ; date:3.2022
Journal of high energy physics ; 2022, Heft 3 (16.3.2022), 1-30, 3.2022

Creator: Berman, David
Fischbacher, Thomas
Inverso, Gianluca

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2022)097

URN: urn:nbn:de:101:1-2022060918485537965418

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

Last update: 15.08.2025, 7:27 AM CEST

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Berman, David
Fischbacher, Thomas
Inverso, Gianluca
SpringerLink (Online service)

Other Objects (12)

$N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity$

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

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

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

$Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity$

Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity

$$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds$

$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds

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

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

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

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

$A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB$

A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB

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

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

$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

$N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity$

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

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

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

$Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity$

Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity

$$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds$

$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds

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

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

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

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

$A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB$

A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB

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

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

$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

$N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity$

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

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

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

$Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity$

Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity

$$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds$

$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds

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

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

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

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

$A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB$

A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB

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

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

$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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New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

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Other Objects (12)

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity

$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds

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

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

A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB

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

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

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

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity

$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds

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

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

A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB

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

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

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

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

Properties of the new N $$ \mathcalN} $$ = 1 AdS4 vacuum of maximal supergravity

$ \mathcalN} $ =1 SUSY AdS4 vacua in IIB SUGRA on group manifolds

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

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

A method to find N $$ \mathcalN} $$ = 1 AdS4 vacua in type IIB

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

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

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

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