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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Kaluza-Klein fermion mass matrices from exceptional field theory and N $$ \mathcalN} $$ = 1 spectra ; volume:2021 ; number:3 ; day:15 ; month:3 ; year:2021 ; pages:1-44 ; date:3.2021
Journal of high energy physics ; 2021, Heft 3 (15.3.2021), 1-44, 3.2021

Creator: Cesàro, Mattia
Varela, Oscar

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2021)138

URN: urn:nbn:de:101:1-2021050319051794995547

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

Last update: 14.08.2025, 10:54 AM CEST

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Cesàro, Mattia
Varela, Oscar
SpringerLink (Online service)

Other Objects (12)

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

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

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

$Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories$

Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories

$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)

$7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory$

7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory

$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

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

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

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

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

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

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

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

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

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

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

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

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

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

$Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories$

Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories

$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)

$7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory$

7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory

$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

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

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

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

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

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

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

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

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

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

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

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

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

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

$Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories$

Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories

$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)

$7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory$

7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory

$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

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

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

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

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

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

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

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

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

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

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

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

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Other Objects (12)

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

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories

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

7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory

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

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

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

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

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

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

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

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

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories

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

7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory

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

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

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

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

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

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

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

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

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Exceptional moduli spaces for exceptional N $$ \mathcalN} $$ = 3 theories

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

7-dimensional N $$ \mathcalN} $$ : = 2 consistent truncations using SL(5) exceptional field theory

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

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

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

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

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

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

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

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