Correlators between Wilson loop and chiral operators in N=2 $$ \mathcalN}=2 $$ conformal gauge theories

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Correlators between Wilson loop and chiral operators in N=2 $$ \mathcalN}=2 $$ conformal gauge theories ; volume:2018 ; number:3 ; day:30 ; month:3 ; year:2018 ; pages:1-38 ; date:3.2018
Journal of high energy physics ; 2018, Heft 3 (30.3.2018), 1-38, 3.2018

Classification: Physik

Creator: Billò, M.

Contributor: Galvagno, F.
Gregori, P.
Lerda, A.
SpringerLink (Online service)

DOI: 10.1007/JHEP03(2018)193

URN: urn:nbn:de:101:1-2018060822090665278083

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2031, 7:24 AM CEST

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Billò, M.
Galvagno, F.
Gregori, P.
Lerda, A.
SpringerLink (Online service)

Other Objects (12)

$Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories$

Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

$Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories$

Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories

$Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group$

Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group

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

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

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

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

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

$Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators$

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories$

Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

$Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories$

Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories

$Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group$

Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group

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

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

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

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

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

$Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators$

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories$

Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

$Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories$

Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories

$Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group$

Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group

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

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

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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

$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

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

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

$Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators$

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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Correlators between Wilson loop and chiral operators in N=2 $$ \mathcalN}=2 $$ conformal gauge theories

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Other Objects (12)

Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories

N $$ \mathcalN} $$ = 1 conformal dualities

Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories

Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group

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

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

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

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories

N $$ \mathcalN} $$ = 1 conformal dualities

Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories

Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group

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

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

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

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Two-point correlators in non-conformal N $$ \mathcalN} $$ = 2 gauge theories

N $$ \mathcalN} $$ = 1 conformal dualities

Wilson loop correlators at strong coupling in N $$ \mathcalN} $$ = 2 quiver gauge theories

Modular invariant holographic correlators for N $$ \mathcalN} $$ = 4 SYM with general gauge group

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

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

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

Ten dimensional symmetry of N $$ \mathcalN} $$ = 4 SYM correlators

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

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