Magnetic quivers, Higgs branches and 6d N : = 1 , 0 $$ \mathcalN} = \left(1,\kern0.5em 0\right) $$ theories

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Weitere Titel: 1 , 0 $$ \mathcalN}
\left(1,\kern0.5em 0\right) $$ theories

Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: Magnetic quivers, Higgs branches and 6d N ; volume:2019 ; number:6 ; day:14 ; month:6 ; year:2019 ; pages:1-55 ; date:6.2019
Journal of high energy physics ; 2019, Heft 6 (14.6.2019), 1-55, 6.2019

Urheber: Cabrera, Santiago
Hanany, Amihay
Sperling, Marcus

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2019)071

URN: urn:nbn:de:101:1-2020020223351069742935

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

Letzte Aktualisierung: 14.08.2025, 10:57 MESZ

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Beteiligte

Cabrera, Santiago
Hanany, Amihay
Sperling, Marcus
SpringerLink (Online service)

Ähnliche Objekte (12)

$Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories$

Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories

$Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups$

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

$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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

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

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

$Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories$

Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories

$Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups$

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

$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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

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

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

$Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories$

Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories

$Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups$

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

$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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

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

IIB duals of D = 3 $ \mathcalN} = 4 $ circular 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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Magnetic quivers, Higgs branches and 6d N : = 1 , 0 $$ \mathcalN} = \left(1,\kern0.5em 0\right) $$ theories

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Ähnliche Objekte (12)

Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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

Erratum to: Magnetic quivers, Higgs branches and 6d N $$ \mathcalN} $$ : = (1, 0) theories

Magnetic quivers, Higgs branches, and 6d N $$ \mathcalN} $$ : = (1, 0) theories — orthogonal and symplectic gauge groups

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

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

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