Dual theory for maximally N $$ \mathcalN} $$ extended flat supergravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Dual theory for maximally N $$ \mathcalN} $$ extended flat supergravity ; volume:2022 ; number:5 ; day:27 ; month:5 ; year:2022 ; pages:1-21 ; date:5.2022
Journal of high energy physics ; 2022, Heft 5 (27.5.2022), 1-21, 5.2022

Creator: Banerjee, Nabamita
Bhattacharjee, Arindam
Biswas, Surajit
Neogi, Turmoli

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2022)179

URN: urn:nbn:de:101:1-2022073006112502460704

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

Last update: 2025-08-15T07:25:14+0200

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Banerjee, Nabamita
Bhattacharjee, Arindam
Biswas, Surajit
Neogi, Turmoli
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity$

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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

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

$Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions$

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

$N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene$

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

$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

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

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

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

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

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

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity$

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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

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

$Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions$

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

$N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene$

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

$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

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

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

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

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

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

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity$

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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

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

$Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions$

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

$N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene$

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

$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

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

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

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

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

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

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

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Dual theory for maximally N $$ \mathcalN} $$ extended flat supergravity

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Other Objects (12)

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

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

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

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

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

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

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

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

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 extended MacDowell-Mansouri supergravity

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

Maximally N $$ \mathcalN} $$ -extended super-BMS3 algebras and generalized 3D gravity solutions

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

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

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

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

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

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