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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers ; volume:2024 ; number:4 ; day:11 ; month:4 ; year:2024 ; pages:1-33 ; date:4.2024
Journal of high energy physics ; 2024, Heft 4 (11.4.2024), 1-33, 4.2024

Creator: Beccaria, M.
Korchemsky, G.P

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP04(2024)054

URN: urn:nbn:de:101:1-2406251036211.908922954452

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

Last update: 14.08.2025, 10:53 AM CEST

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Beccaria, M.
Korchemsky, G.P
SpringerLink (Online service)

Other Objects (12)

$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

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

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

$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

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

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

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

$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

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

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

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

$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

$Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories$

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

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

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Other Objects (12)

Chiral 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

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

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

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

Chiral 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

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

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

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

Chiral 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

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

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

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

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

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

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

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

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