Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description ; volume:2013 ; number:11 ; day:14 ; month:11 ; year:2013 ; pages:1-30 ; date:11.2013
Journal of high energy physics ; 2013, Heft 11 (14.11.2013), 1-30, 11.2013

Creator: Petropoulos, P. Marios
Sfetsos, Konstadinos
Siampos, Konstadinos

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP11(2013)118

URN: urn:nbn:de:101:1-2019101707251535726457

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

Last update: 15.08.2025, 7:30 AM CEST

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Petropoulos, P. Marios
Sfetsos, Konstadinos
Siampos, Konstadinos
SpringerLink (Online service)

Other Objects (12)

$Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description$

Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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

$Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description$

Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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

$Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description$

Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

$Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories$

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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

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Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

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Other Objects (12)

Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

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

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