A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations ; volume:2022 ; number:4 ; day:19 ; month:4 ; year:2022 ; pages:1-14 ; date:4.2022
Journal of high energy physics ; 2022, Heft 4 (19.4.2022), 1-14, 4.2022

Urheber: Bristow, Devin D.
Caporaletti, John H.
Cianciara, Aleksander J.
Gates, S. James
Levine, Delina
Yerger, Gabriel

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2022)104

URN: urn:nbn:de:101:1-2022070306415618826966

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

Letzte Aktualisierung: 15.08.2025, 07:32 MESZ

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Beteiligte

Bristow, Devin D.
Caporaletti, John H.
Cianciara, Aleksander J.
Gates, S. James
Levine, Delina
Yerger, Gabriel
SpringerLink (Online service)

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A note on exemplary off-shell constructions of 4D, N $$ \mathcalN} $$ = 2 supersymmetry representations

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Ähnliche Objekte (12)

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

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

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

Off-shell form factor in N $$ \mathcalN} $$ =4 sYM at three loops

Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

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

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

Off-shell N $$ \mathcalN} $$ = 2 linear multiplets in five dimensions

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

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d

Basis for non-factorizable superamplitudes in N $$ \mathcalN} $$ = 1 supersymmetry

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Unconstrained off-shell superfield formulation of 4D, N $$ \mathcalN} $$ = 2 supersymmetric higher spins

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On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

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Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

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