Magnetic quivers and line defects — On a duality between 3d N $$ \mathcalN} $$ : = 4 unitary and orthosymplectic quivers

to related objects

Alternative title: 4 unitary and orthosymplectic quivers

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Magnetic quivers and line defects — On a duality between 3d N $$ \mathcalN} $$ ; volume:2022 ; number:2 ; day:21 ; month:2 ; year:2022 ; pages:1-72 ; date:2.2022
Journal of high energy physics ; 2022, Heft 2 (21.2.2022), 1-72, 2.2022

Creator: Nawata, Satoshi
Sperling, Marcus
Wang, Hao Ellery
Zhong, Zhenghao

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2022)174

URN: urn:nbn:de:101:1-2022052420370246545051

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

Last update: 15.08.2025, 7:38 AM CEST

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Nawata, Satoshi
Sperling, Marcus
Wang, Hao Ellery
Zhong, Zhenghao
SpringerLink (Online service)

Other Objects (12)

$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

$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

$Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers$

Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers

$Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities$

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

$Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers$

Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers

$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

$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

$Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers$

Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers

$Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities$

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

$Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers$

Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers

$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

$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

$Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers$

Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers

$Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities$

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

$Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers$

Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers

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Magnetic quivers and line defects — On a duality between 3d N $$ \mathcalN} $$ : = 4 unitary and orthosymplectic quivers

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Other Objects (12)

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

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

Chiral 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

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

Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers

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

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

Chiral 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

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

Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers

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

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

Chiral 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

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

Field theory aspects of non-Abelian T-duality and N $$ \mathcalN} $$ =2 linear quivers

Multi-cover skeins, quivers, and 3d N $$ \mathcalN} $$ = 2 dualities

Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers

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