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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: N $$ \mathcalN} $$ = (1, 1) supersymmetric AdS3 in 10 dimensions ; volume:2022 ; number:3 ; day:17 ; month:3 ; year:2022 ; pages:1-43 ; date:3.2022
Journal of high energy physics ; 2022, Heft 3 (17.3.2022), 1-43, 3.2022

Creator: Macpherson, Niall T.
Tomasiello, Alessandro

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2022)112

URN: urn:nbn:de:101:1-2022061019283311415241

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

Last update: 15.08.2025, 7:36 AM CEST

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Macpherson, Niall T.
Tomasiello, Alessandro
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

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

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

Supersymmetric black hole hair and AdS3 × S3

Integrable supersymmetric deformations of AdS3 × S3 × T4

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

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

Supersymmetric AdS3 supergravity backgrounds and holography

$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

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$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

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

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

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

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

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

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

Supersymmetric black hole hair and AdS3 × S3

Integrable supersymmetric deformations of AdS3 × S3 × T4

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

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

Supersymmetric AdS3 supergravity backgrounds and holography

$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

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$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

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

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

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

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

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

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

Supersymmetric black hole hair and AdS3 × S3

Integrable supersymmetric deformations of AdS3 × S3 × T4

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

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

Supersymmetric AdS3 supergravity backgrounds and holography

$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

$N $$ \mathcalN} $$ = 2 supersymmetric S-folds$

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

$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

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

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Other Objects (12)

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

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

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

Supersymmetric black hole hair and AdS3 × S3

Integrable supersymmetric deformations of AdS3 × S3 × T4

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

Supersymmetric AdS3 supergravity backgrounds and holography

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

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

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

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

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

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

Supersymmetric black hole hair and AdS3 × S3

Integrable supersymmetric deformations of AdS3 × S3 × T4

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

Supersymmetric AdS3 supergravity backgrounds and holography

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

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

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

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

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

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

Supersymmetric black hole hair and AdS3 × S3

Integrable supersymmetric deformations of AdS3 × S3 × T4

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

Supersymmetric AdS3 supergravity backgrounds and holography

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

N $$ \mathcalN} $$ = 2 supersymmetric S-folds

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

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