M -strings and AdS3 solutions to M-theory with small N $$ \mathcalN} $$ = (0, 4) supersymmetry

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: M -strings and AdS3 solutions to M-theory with small N $$ \mathcalN} $$ = (0, 4) supersymmetry ; volume:2020 ; number:8 ; day:25 ; month:8 ; year:2020 ; pages:1-29 ; date:8.2020
Journal of high energy physics ; 2020, Heft 8 (25.8.2020), 1-29, 8.2020

Creator: Lozano, Yolanda
Nunez, Carlos
Ramirez, Anayeli
Speziali, Stefano

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2020)118

URN: urn:nbn:de:101:1-2020101423095125303322

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

Last update: 14.08.2025, 10:52 AM CEST

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Lozano, Yolanda
Nunez, Carlos
Ramirez, Anayeli
Speziali, Stefano
SpringerLink (Online service)

Other Objects (12)

$AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry$

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals$

Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals

$N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions$

N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB$

New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB

$AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry$

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals$

Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals

$N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions$

N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB$

New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB

$AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry$

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

$Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry$

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

$Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3$

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry$

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

$Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals$

Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals

$N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions$

N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions

$On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions$

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

$Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity$

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB$

New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB

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M -strings and AdS3 solutions to M-theory with small N $$ \mathcalN} $$ = (0, 4) supersymmetry

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Other Objects (12)

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals

N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals

N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB

AdS3 solutions in massive IIA with small N $$ \mathcalN} $$ = (4, 0) supersymmetry

Nonlocal N = 1 $$ \mathcalN}=1 $$ supersymmetry

Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Nonlinear N = 2 $$ \mathcalN}=2 $$ global supersymmetry

Twisted N $$ \mathcalN} $$ = 1 SCFTs and their AdS3 duals

N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions

On N $$ \mathcalN} $$ = 4 supersymmetry enhancements in three dimensions

Supersymmetry anomalies in N = 1 $$ \mathcalN}=1 $$ conformal supergravity

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB

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