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

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

Umfang: Online-Ressource, 1 online resource.

Sprache: Englisch

Erschienen in: Mixed moduli in 3d N $$ \mathcalN} $$ = 4 higher-genus quivers ; volume:2023 ; number:5 ; day:16 ; month:5 ; year:2023 ; pages:1-58 ; date:5.2023
Journal of high energy physics ; 2023, Heft 5 (16.5.2023), 1-58, 5.2023

Urheber: Lavdas, Ioannis
Floch, Bruno Le

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2023)124

URN: urn:nbn:de:101:1-2023110609084023415805

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

Letzte Aktualisierung: 14.08.2025, 10:47 MESZ

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Beteiligte

Lavdas, Ioannis
Floch, Bruno Le
SpringerLink (Online service)

Ähnliche Objekte (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

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

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

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

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

$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

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

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

$Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions$

Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions

$Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography$

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

$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

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

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

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

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

$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

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

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

$Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions$

Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions

$Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography$

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

$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

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

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

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

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

$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

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

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

$Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions$

Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions

$Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography$

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

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

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Ähnliche Objekte (12)

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

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

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

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

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

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

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

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

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

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

Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

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

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

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

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

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

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

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

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

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

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

Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

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

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

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

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

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

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

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

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

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

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

Phases of N $$ \mathcalN} $$ = 1 quivers in 2 + 1 dimensions

Strong-coupling results for N $$ \mathcalN} $$ = 2 superconformal quivers and holography

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