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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers ; volume:2021 ; number:5 ; day:21 ; month:5 ; year:2021 ; pages:1-46 ; date:5.2021
Journal of high energy physics ; 2021, Heft 5 (21.5.2021), 1-46, 5.2021

Creator: Galvagno, Francesco
Preti, Michelangelo

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2021)201

URN: urn:nbn:de:101:1-2021111520422312483351

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

Last update: 15.08.2025, 7:31 AM CEST

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Galvagno, Francesco
Preti, Michelangelo
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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

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

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

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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

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

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

$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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Other Objects (12)

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

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

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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

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

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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

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

Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

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

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

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

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