N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell ; volume:2015 ; number:4 ; day:14 ; month:4 ; year:2015 ; pages:1-34 ; date:4.2015
Journal of high energy physics ; 2015, Heft 4 (14.4.2015), 1-34, 4.2015

Classification: Physik

Creator: Sloane, Peter

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2015)062

URN: urn:nbn:de:1111-2018041513744

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:59 AM CEST

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Sloane, Peter
SpringerLink (Online service)

Other Objects (12)

$Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity$

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

$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

$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

Off-shell Poincaré supergravity

$New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory$

New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory

$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

$Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity$

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

$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

$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

Off-shell Poincaré supergravity

$New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory$

New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory

$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

$Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity$

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

$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

$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

Off-shell Poincaré supergravity

$New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory$

New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory

$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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N=2 $$ \mathcalN}=2 $$ dilaton-Weyl multiplets in 5D and Nishino-Rajpoot supergravity off-shell

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Other Objects (12)

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

Off-shell Poincaré supergravity

New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory

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

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

Off-shell Poincaré supergravity

New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory

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

Hyper-dilaton Weyl multiplet of 4D, N $$ \mathcalN} $$ = 2 conformal supergravity

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

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

Off-shell Poincaré supergravity

New BPS solitons in N $$ \mathcalN} $$ = 4 gauged supergravity and black holes in Einstein-Yang-Mills-dilaton theory

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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