Nilpotent chiral superfield in N = 2 $$ \mathcalN}=2 $$ supergravity and partial rigid supersymmetry breaking

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Nilpotent chiral superfield in N = 2 $$ \mathcalN}=2 $$ supergravity and partial rigid supersymmetry breaking ; volume:2016 ; number:3 ; day:15 ; month:3 ; year:2016 ; pages:1-25 ; date:3.2016
Journal of high energy physics ; 2016, Heft 3 (15.3.2016), 1-25, 3.2016

Creator: Kuzenko, Sergei M.

Contributor: Tartaglino-Mazzucchelli, Gabriele
SpringerLink (Online service)

DOI: 10.1007/JHEP03(2016)092

URN: urn:nbn:de:1111-2016031814108

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:59 AM CEST

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Kuzenko, Sergei M.
Tartaglino-Mazzucchelli, Gabriele
SpringerLink (Online service)

Other Objects (12)

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Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

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

$Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity$

Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity

$Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet$

Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet

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

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

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$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

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Properties of nilpotent supergravity

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

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

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

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

$Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity$

Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity

$Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet$

Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet

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

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

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$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

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Properties of nilpotent supergravity

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

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

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity$

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

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

$Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity$

Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity

$Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet$

Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet

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

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

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$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

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Properties of nilpotent supergravity

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

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

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Nilpotent chiral superfield in N = 2 $$ \mathcalN}=2 $$ supergravity and partial rigid supersymmetry breaking

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Other Objects (12)

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity

Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet

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

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

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

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

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Properties of nilpotent supergravity

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

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity

Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet

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

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

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

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

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Properties of nilpotent supergravity

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

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Behaviors of two supersymmetry breaking scales in N $$ \mathcalN} $$ : = 2 supergravity

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

Supersymmetry constraints on U-duality invariant deformations of N $$ \mathcalN} $$ ≥ 5 supergravity

Nilpotent N=1 $$ \mathcalN}=1 $$ tensor multiplet

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

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

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

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

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Properties of nilpotent supergravity

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

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