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

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Alternative title: 1 Kaluza-Klein superspace

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 4D N $$ \mathcalN} $$ ; volume:2020 ; number:9 ; day:11 ; month:9 ; year:2020 ; pages:1-51 ; date:9.2020
Journal of high energy physics ; 2020, Heft 9 (11.9.2020), 1-51, 9.2020

Creator: Becker, Katrin
Butter, Daniel

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP09(2020)091

URN: urn:nbn:de:101:1-2020103123181755884767

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

Last update: 15.08.2025, 7:38 AM CEST

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Becker, Katrin
Butter, Daniel
SpringerLink (Online service)

Other Objects (12)

$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

$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

$The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)$

The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)

$Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra$

Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra

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

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

$Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs$

Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs

$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

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

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

$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

$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

$The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)$

The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)

$Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra$

Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra

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

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

$Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs$

Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs

$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

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

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

$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

$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

$The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)$

The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)

$Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra$

Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra

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

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

$Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs$

Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs

$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

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

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

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

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Other Objects (12)

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

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

The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)

Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra

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

Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

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

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

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

The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)

Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra

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

Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

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

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

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

The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7)

Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra

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

Geometric classification of 4d N=2 $$ \mathcalN}=2 $$ SCFTs

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

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

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