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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: The complete Kaluza-Klein spectra of N $$ \mathcalN} $$ = 1 and N $$ \mathcalN} $$ = 0 M-theory on AdS 4 × (squashed S 7) ; volume:2024 ; number:2 ; day:20 ; month:2 ; year:2024 ; pages:1-85 ; date:2.2024
Journal of high energy physics ; 2024, Heft 2 (20.2.2024), 1-85, 2.2024

Classification: Physik

Creator: Karlsson, Joel
Nilsson, Bengt E. W.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2024)144

URN: urn:nbn:de:101:1-2404291359169.678197715430

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

Last update: 14.08.2025, 10:59 AM CEST

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Karlsson, Joel
Nilsson, Bengt E. W.
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

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

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

$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

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

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

$Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds$

Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

$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

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

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

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

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

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

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

$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

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

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

$Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds$

Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

$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

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

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

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

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

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

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

$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

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

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

$Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds$

Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

$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

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

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Other Objects (12)

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

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

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

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

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

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

Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

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

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

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

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

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

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

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

Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

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

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

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

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

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

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

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

Generalised structures for N = 1 $$ \mathcalN}=1 $$ AdS backgrounds

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

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