4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups ; volume:2017 ; number:3 ; day:28 ; month:3 ; year:2017 ; pages:1-43 ; date:3.2017
Journal of high energy physics ; 2017, Heft 3 (28.3.2017), 1-43, 3.2017

Classification: Physik

Creator: Argyres, Philip C.

Contributor: Martone, Mario
SpringerLink (Online service)

DOI: 10.1007/JHEP03(2017)145

URN: urn:nbn:de:1111-201704163585

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:31 AM CEST

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Argyres, Philip C.
Martone, Mario
SpringerLink (Online service)

Other Objects (12)

$Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

$Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories$

Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories

$Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD$

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

$4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma$

4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma

$Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories

$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

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities$

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

$Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

$Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories$

Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories

$Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD$

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

$4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma$

4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma

$Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories

$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

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities$

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

$Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

$Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories$

Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories

$Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD$

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

$4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma$

4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma

$Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories

$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

$Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM$

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM$

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

$4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities$

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

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4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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Other Objects (12)

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma

Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories

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

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma

Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories

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

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

Quantum integrability of N=2 $$ \mathcalN}=2 $$ 4d gauge theories

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

4d N $$ \mathcalN} $$ = 1 quiver gauge theories and the An Bailey lemma

Sequential deconfinement and self-dualities in 4d N $$ \mathcalN} $$ = 1 gauge theories

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

Domain walls in 4d N $$ \mathcalN} $$ = 1 SYM

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

Splitting interfaces in 4d N $$ \mathcalN} $$ = 4 SYM

4d N $$ \mathcalN} $$ = 1 dualities from 5d dualities

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