4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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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 = 3 $$ \mathcalN}=3 $$ indices via discrete gauging ; volume:2018 ; number:10 ; day:19 ; month:10 ; year:2018 ; pages:1-34 ; date:10.2018
Journal of high energy physics ; 2018, Heft 10 (19.10.2018), 1-34, 10.2018

Creator: Bourton, Thomas
Pini, Alessandro
Pomoni, Elli

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP10(2018)131

URN: urn:nbn:de:101:1-2021082521303916939986

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

Last update: 14.08.2025, 10:51 AM CEST

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Bourton, Thomas
Pini, Alessandro
Pomoni, Elli
SpringerLink (Online service)

Other Objects (12)

4d N=3 indices via discrete gauging

$Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities$

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

$Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric gauge theories$

Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric 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)

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

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

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

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

$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

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

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

$Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT$

Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT

4d N=3 indices via discrete gauging

$Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities$

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

$Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric gauge theories$

Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric 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)

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

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

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

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

$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

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

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

$Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT$

Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT

4d N=3 indices via discrete gauging

$Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities$

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

$Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric gauge theories$

Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric 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)

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

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

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

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

$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

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

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

$Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT$

Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT

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4d N = 3 $$ \mathcalN}=3 $$ indices via discrete gauging

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Other Objects (12)

4d N=3 indices via discrete gauging

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric gauge theories

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

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

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

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

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

Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT

4d N=3 indices via discrete gauging

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric gauge theories

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

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

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

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

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

Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT

4d N=3 indices via discrete gauging

Gauging and decoupling in 3d N $$ \mathcalN} $$ = 2 dualities

Discrete gauging in Coulomb branches of three dimensional N=4 $$ \mathcalN}=4 $$ supersymmetric gauge theories

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

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

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

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

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

Exploring the minimal 4D N = 1 $$ \mathcalN}=1 $$ SCFT

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