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

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: New N $$ \mathcalN} $$ = (0, 4) AdS3 near-horizons in Type IIB ; volume:2021 ; number:4 ; day:6 ; month:4 ; year:2021 ; pages:1-34 ; date:4.2021
Journal of high energy physics ; 2021, Heft 4 (6.4.2021), 1-34, 4.2021

Urheber: Faedo, Federico
Lozano, Yolanda
Petri, Nicolò

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2021)028

URN: urn:nbn:de:101:1-2021102404254997041090

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

Letzte Aktualisierung: 15.08.2025, 07:26 MESZ

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Beteiligte

Faedo, Federico
Lozano, Yolanda
Petri, Nicolò
SpringerLink (Online service)

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

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

$N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes$

N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes

$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

$IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers$

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

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

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

$All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions$

All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions

$N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces$

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$On $\mathcalN} = 2$ truncations of IIB on T 1,1$

On $\mathcalN} = 2$ truncations of IIB on T 1,1

$Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds$

Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds

$Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons$

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

$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

$N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes$

N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes

$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

$IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers$

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

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

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

$All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions$

All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions

$N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces$

N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces

$On $\mathcalN} = 2$ truncations of IIB on T 1,1$

On $\mathcalN} = 2$ truncations of IIB on T 1,1

$Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds$

Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds

$Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons$

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

$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

$N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes$

N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes

$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

$IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers$

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

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

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

$All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions$

All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions

$N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces$

N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces

$On $\mathcalN} = 2$ truncations of IIB on T 1,1$

On $\mathcalN} = 2$ truncations of IIB on T 1,1

$Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds$

Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds

$Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons$

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

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

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Ähnliche Objekte (12)

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

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

N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes

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

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

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

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

All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions

N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces

On $\mathcalN} = 2$ truncations of IIB on T 1,1

Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

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

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

N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes

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

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

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

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

All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions

N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces

On $\mathcalN} = 2$ truncations of IIB on T 1,1

Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

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

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

N $$ \mathcalN} $$ = (0, 2) AdS3 solutions of type IIB and F-theory with generic fluxes

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

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

IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers

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

All N $$ \mathcalN} $$ = (8, 0) AdS3 solutions in 10 and 11 dimensions

N $$ \mathcalN} $$ = (2, 2) AdS3 from D3-branes wrapped on Riemann surfaces

On $\mathcalN} = 2$ truncations of IIB on T 1,1

Marginal deformations of a class of AdS3 N $$ \mathcalN} $$ = (0, 4) holographic backgrounds

Dynamical symmetry enhancement near N $$ \mathcalN} $$ = 2, D = 4 gauged supergravity horizons

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