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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The planar limit of N $$ \mathcalN} $$ = 2 chiral correlators ; volume:2021 ; number:8 ; day:9 ; month:8 ; year:2021 ; pages:1-20 ; date:8.2021
Journal of high energy physics ; 2021, Heft 8 (9.8.2021), 1-20, 8.2021

Creator: Fiol, Bartomeu
Fukelman, Alan Rios

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2021)032

URN: urn:nbn:de:101:1-2021103120434147331958

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

Last update: 15.08.2025, 7:27 AM CEST

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Fiol, Bartomeu
Fukelman, Alan Rios
SpringerLink (Online service)

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

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

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

$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$

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

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

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

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

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

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

$All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM$

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

$Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model$

Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model

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

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

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

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

$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

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

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

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

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

$All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM$

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

$Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model$

Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model

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

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

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

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

$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

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

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

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

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

$All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM$

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

$Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model$

Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model

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

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Other Objects (12)

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

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

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

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

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

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model

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

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

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

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

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

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model

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

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

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

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

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

All three-loop four-point correlators of half-BPS operators in planar N $$ \mathcalN} $$ : = 4 SYM

Correlators in the N = 2 $$ \mathcalN}=2 $$ supersymmetric SYK model

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