Wilson loops and its correlators with chiral operators in N $$ \mathcalN} $$ = 2, 4 SCFT at large N

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Wilson loops and its correlators with chiral operators in N $$ \mathcalN} $$ = 2, 4 SCFT at large N ; volume:2018 ; number:3 ; day:26 ; month:3 ; year:2018 ; pages:1-24 ; date:3.2018
Journal of high energy physics ; 2018, Heft 3 (26.3.2018), 1-24, 3.2018

Classification: Physik

Creator: Sysoeva, E.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2018)155

URN: urn:nbn:de:101:1-2018053105084799201626

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:37 AM CEST

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Sysoeva, E.
SpringerLink (Online service)

Other Objects (12)

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$The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators$

The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

$A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators$

A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

$Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace$

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

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

$Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop$

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$On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation$

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

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$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

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

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

$The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators$

The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

$A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators$

A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

$Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace$

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

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

$Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop$

Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop

$On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation$

On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation

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

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

$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

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

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

$The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators$

The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

$A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators$

A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

$Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace$

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

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

$Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop$

Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop

$On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation$

On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation

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

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

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$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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Wilson loops and its correlators with chiral operators in N $$ \mathcalN} $$ = 2, 4 SCFT at large N

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Other Objects (12)

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

The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop

On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation

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

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

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

The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop

On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation

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

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

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

The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

A derivation of the planar limit of N $$ \mathcalN} $$ = 2 chiral correlators

Smooth Wilson loops in N = 4 $$ \mathcalN}=4 $$ non-chiral superspace

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

Double scaling limit of N $$ \mathcalN} $$ = 2 chiral correlators with Maldacena-Wilson loop

On the large R-charge N $$ \mathcalN} $$ = 2 chiral correlators and the Toda equation

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

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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