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

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 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

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

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2022)104

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

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

Last update: 15.08.2025, 7:32 AM CEST

Data provider

This object is provided by:
Deutsche Nationalbibliothek. If you have any questions about the object, please contact the data provider.

Show original at data provider

Associated

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

Other Objects (12)

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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$

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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$

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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$

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

Cultural heritage institutions wishing to register will find more information here.

Fields marked * need to be filled in.

Username*

Please enter your username

Email*

Please enter your email address

Please do not fill this field

First name

Last name

Password*

Please enter your password

Confirm password*

Please enter the same password

I have read the terms of use and the privacy policy for the collection of personal data and accept them. *

This field is required.

I would like to subscribe to the newsletter of the Deutsche Digitale Bibliothek. See newsletter subscription info.

Account created

Your "My DDB" account has been successfully created. Before you can log in to your account, you must click the confirmation link in the message we just sent to the email address you provided.

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

Object Details

References and Relationships

Contributors, Places and Time

Further information

Data provider

Associated

Other Objects (12)

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

Related objects

Reset password