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

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: IIB duals of D = 3 $ \mathcalN} = 4 $ circular quivers ; volume:2012 ; number:12 ; day:10 ; month:12 ; year:2012 ; pages:1-47 ; date:12.2012
Journal of high energy physics ; 2012, Heft 12 (10.12.2012), 1-47, 12.2012

Klassifikation: Physik

Urheber: Assel, Benjamin
Bachas, Costas
Estes, John
Gomis, Jaume

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP12(2012)044

URN: urn:nbn:de:101:1-2019060823314366686642

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

Letzte Aktualisierung: 14.08.2025, 10:54 MESZ

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Beteiligte

Assel, Benjamin
Bachas, Costas
Estes, John
Gomis, Jaume
SpringerLink (Online service)

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$Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals$

Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals

$Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals$

Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals

$Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers$

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

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

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

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

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

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

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

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

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

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers$

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

$Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers$

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

$N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers$

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

$Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers$

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

$Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals$

Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals

$Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals$

Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals

$Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers$

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

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

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

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

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

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

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

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

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

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers$

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

$Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers$

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

$N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers$

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

$Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers$

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

$Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals$

Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals

$Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals$

Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals

$Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers$

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

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

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

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

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

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

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

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

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

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

$Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers$

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

$Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers$

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

$N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers$

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

$Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers$

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

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

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Ähnliche Objekte (12)

Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals

Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

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

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

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

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

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals

Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

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

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

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

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

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

Three-dimensional N = 4 $$ \mathcalN}=4 $$ linear quivers and non-Abelian T-duals

Magnons and spikes for N $$ \mathcalN} $$ = 2 linear quivers and their non-Abelian T-duals

Factorised 3d N $$ \mathcalN} $$ = 4 orthosymplectic quivers

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

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

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

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

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

Large N correlation functions N $$ \mathcalN} $$ = 2 superconformal quivers

Electrostatic description of 3d N $$ \mathcalN} $$ = 4 linear quivers

N $$ \mathcalN} $$ = 1 conformal dualities from unoriented chiral quivers

Monopoles and dualities in 3d N $$ \mathcalN} $$ = 2 quivers

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