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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry ; volume:2017 ; number:6 ; day:12 ; month:6 ; year:2017 ; pages:1-38 ; date:6.2017
Journal of high energy physics ; 2017, Heft 6 (12.6.2017), 1-38, 6.2017

Classification: Physik

Creator: Antoniadis, Ignatios

Contributor: Derendinger, Jean-Pierre
Markou, Chrysoula
SpringerLink (Online service)

DOI: 10.1007/JHEP06(2017)052

URN: urn:nbn:de:1111-201711051001

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:27 AM CEST

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Antoniadis, Ignatios
Derendinger, Jean-Pierre
Markou, Chrysoula
SpringerLink (Online service)

Other Objects (12)

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$Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry$

Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry

$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$

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

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

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

$Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry$

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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

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

$N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography$

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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

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

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

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

$Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry$

Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry

$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

$Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry$

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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

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

$N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography$

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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

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

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

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

$Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry$

Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry

$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

$Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry$

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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

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

$N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography$

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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

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

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

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Other Objects (12)

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

Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry

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

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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

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

Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry

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

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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

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

Deformation of d = 4, N $$ \mathcalN} $$ ≥ 5 supergravities breaks nonlinear local supersymmetry

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

Witten anomaly in 4d heterotic compactificaitons with N $$ \mathcalN} $$ = 2 supersymmetry

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

N $$ \mathcalN} $$ = 2 supersymmetry in the twistor description of higher-spin holography

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

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