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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Stringy N $$ \mathcalN} $$ = (2, 2) holography for AdS3 ; volume:2018 ; number:1 ; day:30 ; month:1 ; year:2018 ; pages:1-37 ; date:1.2018
Journal of high energy physics ; 2018, Heft 1 (30.1.2018), 1-37, 1.2018

Classification: Physik

Creator: Datta, Shouvik

Contributor: Eberhardt, Lorenz
Gaberdiel, Matthias
SpringerLink (Online service)

DOI: 10.1007/JHEP01(2018)146

URN: urn:nbn:de:1111-201803286598

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:48 AM CEST

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Datta, Shouvik
Eberhardt, Lorenz
Gaberdiel, Matthias
SpringerLink (Online service)

Other Objects (12)

Supercharged AdS3 Holography

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

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

$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

AdS3 holography at dimension two

$N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2$

N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2

$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

Aspects of holography in conical AdS3

Spacetime dilaton in AdS3 × X 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

Supercharged AdS3 Holography

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

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

$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

AdS3 holography at dimension two

$N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2$

N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2

$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

Aspects of holography in conical AdS3

Spacetime dilaton in AdS3 × X 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

Supercharged AdS3 Holography

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

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

$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

AdS3 holography at dimension two

$N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2$

N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2

$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

Aspects of holography in conical AdS3

Spacetime dilaton in AdS3 × X 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

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

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Other Objects (12)

Supercharged AdS3 Holography

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

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

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

AdS3 holography at dimension two

N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2

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

Supersymmetric AdS3 supergravity backgrounds and holography

Aspects of holography in conical AdS3

Spacetime dilaton in AdS3 × X 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

Supercharged AdS3 Holography

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

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

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

AdS3 holography at dimension two

N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2

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

Supersymmetric AdS3 supergravity backgrounds and holography

Aspects of holography in conical AdS3

Spacetime dilaton in AdS3 × X 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

Supercharged AdS3 Holography

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

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

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

AdS3 holography at dimension two

N=33 $$ \mathcalN}=\left(3,3\right) $$ holography on AdS3 × (S3 × S3 × S1)/ℤ2

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

Supersymmetric AdS3 supergravity backgrounds and holography

Aspects of holography in conical AdS3

Spacetime dilaton in AdS3 × X 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

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