Gravity duals of N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the 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 N $$ \mathcalN} $$ = 2 SCFTs and asymptotic emergence of the electrostatic description ; volume:2014 ; number:9 ; day:10 ; month:9 ; year:2014 ; pages:1-13 ; date:9.2014
Journal of high energy physics ; 2014, Heft 9 (10.9.2014), 1-13, 9.2014

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

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP09(2014)057

URN: urn:nbn:de:101:1-2019080303384940147077

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

Last update: 15.08.2025, 7:26 AM CEST

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

Other Objects (12)

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

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

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

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

$Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs$

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups$

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$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

$Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs$

Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs$

Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs

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

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

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

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

$Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs$

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups$

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$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

$Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs$

Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs$

Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs

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

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

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

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

$Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs$

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups$

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$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

$Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs$

Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs$

Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs

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

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Other Objects (12)

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

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

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs

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

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

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs

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

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

Reflection groups and 3d N $$ \mathcalN} $$ > 6 SCFTs

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

N $$ \mathcalN} $$ = 5 SCFTs and quaternionic reflection groups

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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

Theories of class S $$ \mathcalS} $$ and new N $$ \mathcalN} $$ = 1 SCFTs

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Dynamical spin chains in 4D N $$ \mathcalN} $$ = 2 SCFTs

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