A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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Alternative title: 2 → N $$ \mathcalN} $$
0 breaking

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: A superfield constraint for N $$ \mathcalN} $$ ; volume:2017 ; number:8 ; day:24 ; month:8 ; year:2017 ; pages:1-23 ; date:8.2017
Journal of high energy physics ; 2017, Heft 8 (24.8.2017), 1-23, 8.2017

Classification: Physik

Creator: Dudas, Emilian

Contributor: Ferrara, S.
Sagnotti, A.
SpringerLink (Online service)

DOI: 10.1007/JHEP08(2017)109

URN: urn:nbn:de:1111-201712083937

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:20 AM CEST

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Dudas, Emilian
Ferrara, S.
Sagnotti, A.
SpringerLink (Online service)

Other Objects (12)

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

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

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

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

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

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

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

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

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality$

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

$A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*$

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

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

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

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

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

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

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

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

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality$

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

$A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*$

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

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

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

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

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

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

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

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

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality$

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

$A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*$

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

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

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

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A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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Other Objects (12)

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

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

N $$ \mathcalN} $$ = 2* Schur indices

N $$ \mathcalN} $$ = 1 conformal dualities

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

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

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

N $$ \mathcalN} $$ = 2* Schur indices

N $$ \mathcalN} $$ = 1 conformal dualities

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

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

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

N $$ \mathcalN} $$ = 2* Schur indices

N $$ \mathcalN} $$ = 1 conformal dualities

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

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

N=2 $$ \mathcalN}=2 $$ Argyres-Douglas theories, N=1 $$ \mathcalN}=1 $$ SQCD and Seiberg duality

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

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

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