Exact 1/N expansion of Wilson loop correlators in N $$ \mathcalN} $$ = 4 Super-Yang-Mills theory

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: Exact 1/N expansion of Wilson loop correlators in N $$ \mathcalN} $$ = 4 Super-Yang-Mills theory ; volume:2021 ; number:7 ; day:1 ; month:7 ; year:2021 ; pages:1-38 ; date:7.2021
Journal of high energy physics ; 2021, Heft 7 (1.7.2021), 1-38, 7.2021

Urheber: Mück, Wolfgang

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2021)001

URN: urn:nbn:de:101:1-2021101302165705495691

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

Letzte Aktualisierung: 15.08.2025, 07:28 MESZ

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Beteiligte

Mück, Wolfgang
SpringerLink (Online service)

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

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

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods$

Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods

$Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory$

Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

$Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory$

Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

$Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB$

Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB

$Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

$N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization$

N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization

$All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

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

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

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods$

Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods

$Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory$

Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

$Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory$

Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

$Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB$

Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB

$Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

$N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization$

N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization

$All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

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

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

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods$

Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods

$Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory$

Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

$Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory$

Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

$Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB$

Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB

$Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

$N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization$

N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization

$All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

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Exact 1/N expansion of Wilson loop correlators in N $$ \mathcalN} $$ = 4 Super-Yang-Mills theory

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Ähnliche Objekte (12)

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

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods

Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB

Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization

All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods

Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB

Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization

All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Integrated correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills and periods

Relations between integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

Exceptionally simple integrated correlators in N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills theory

Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB

Electromagnetic duality for line defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

N $$ \mathcalN} $$ = 4 Super-Yang-Mills correlators at strong coupling from string theory and localization

All-loop Heavy-Heavy-Light-Light correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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