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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Defect multiplets of N = 1 $$ \mathcalN}=1 $$ supersymmetry in 4d ; volume:2018 ; number:1 ; day:9 ; month:1 ; year:2018 ; pages:1-19 ; date:1.2018
Journal of high energy physics ; 2018, Heft 1 (9.1.2018), 1-19, 1.2018

Classification: Physik

Creator: Drukker, N.

Contributor: Shamir, I.
Vergu, C.
SpringerLink (Online service)

DOI: 10.1007/JHEP01(2018)034

URN: urn:nbn:de:1111-201803151537

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:55 AM CEST

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Drukker, N.
Shamir, I.
Vergu, C.
SpringerLink (Online service)

Other Objects (12)

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

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

$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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace$

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

$A 4d N $$ \mathcalN} $$ = 1 Cardy Formula$

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$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

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

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

$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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace$

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

$A 4d N $$ \mathcalN} $$ = 1 Cardy Formula$

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$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

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

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

$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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace$

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

$A 4d N $$ \mathcalN} $$ = 1 Cardy Formula$

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

$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

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

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Other Objects (12)

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

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

4D N $$ \mathcalN} $$ : = 1 Kaluza-Klein superspace

A 4d N $$ \mathcalN} $$ = 1 Cardy Formula

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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