Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity ; volume:2018 ; number:4 ; day:27 ; month:4 ; year:2018 ; pages:1-28 ; date:4.2018
Journal of high energy physics ; 2018, Heft 4 (27.4.2018), 1-28, 4.2018

Classification: Physik

Creator: Bobev, Nikolay

Contributor: Gautason, Friðrik Freyr
Muiden, Jesse van
SpringerLink (Online service)

DOI: 10.1007/JHEP04(2018)148

URN: urn:nbn:de:101:1-2018070220335319659302

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:34 AM CEST

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Bobev, Nikolay
Gautason, Friðrik Freyr
Muiden, Jesse van
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

$New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity$

New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

$N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity$

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

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

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

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$The symmetry of large $ \mathcalN} $ = 4 holography$

The symmetry of large $ \mathcalN} $ = 4 holography

$Even spin N = 4 $$ \mathcalN}=4 $$ holography$

Even spin N = 4 $$ \mathcalN}=4 $$ holography

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

$New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity$

New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

$N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity$

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

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

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

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$The symmetry of large $ \mathcalN} $ = 4 holography$

The symmetry of large $ \mathcalN} $ = 4 holography

$Even spin N = 4 $$ \mathcalN}=4 $$ holography$

Even spin N = 4 $$ \mathcalN}=4 $$ holography

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities$

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

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

$New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity$

New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

$N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity$

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

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

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

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$The symmetry of large $ \mathcalN} $ = 4 holography$

The symmetry of large $ \mathcalN} $ = 4 holography

$Even spin N = 4 $$ \mathcalN}=4 $$ holography$

Even spin N = 4 $$ \mathcalN}=4 $$ holography

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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Precision holography for N=2∗ $$ \mathcalN}={2}^{\ast } $$ on S 4 from type IIB supergravity

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Other Objects (12)

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

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

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

The symmetry of large $ \mathcalN} $ = 4 holography

Even spin N = 4 $$ \mathcalN}=4 $$ holography

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

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

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

The symmetry of large $ \mathcalN} $ = 4 holography

Even spin N = 4 $$ \mathcalN}=4 $$ holography

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 2 AdS4 supergravity, holography and Ward identities

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

New N $$ \mathcalN} $$ = 1 AdS4 solutions of type IIB supergravity

N=2 $$ \mathcalN}=2 $$ supersymmetric AdS4 solutions of type IIB supergravity

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

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

The symmetry of large $ \mathcalN} $ = 4 holography

Even spin N = 4 $$ \mathcalN}=4 $$ holography

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

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