Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1 ; volume:2019 ; number:5 ; day:21 ; month:5 ; year:2019 ; pages:1-61 ; date:5.2019
Journal of high energy physics ; 2019, Heft 5 (21.5.2019), 1-61, 5.2019

Creator: Beccaria, Matteo
Giombi, Simone
Tseytlin, Arkady A.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2019)122

URN: urn:nbn:de:101:1-2019110119393282130287

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

Last update: 15.08.2025, 7:36 AM CEST

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Beccaria, Matteo
Giombi, Simone
Tseytlin, Arkady A.
SpringerLink (Online service)

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

$Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM$

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$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

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Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM

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$Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM$

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Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

$Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory$

Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory

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

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

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

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

$Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM$

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM$

Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM

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

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

$Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM$

Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM

$Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM$

Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM

$Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM$

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

$Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory$

Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory

$Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries$

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

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

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

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

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

$Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM$

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM$

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

$Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM$

Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM

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

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

$Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM$

Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM

$Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM$

Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM

$Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM$

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

$Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N$

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

$Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory$

Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory

$Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries$

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

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Correlators on non-supersymmetric Wilson line in N = 4 $$ \mathcalN}=4 $$ SYM and AdS2/CFT1

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Other Objects (12)

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

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

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM

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

Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM

Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

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

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

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM

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

Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM

Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

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

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

Algebras, traces, and boundary correlators in N $$ \mathcalN} $$ = 4 SYM

Supersymmetric gradient flow in $$\mathcalN}=1$$ N = 1 SYM

Integrated correlators with a Wilson line in N $$ \mathcalN} $$ = 4 SYM

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

Integrated correlators from integrability: Maldacena-Wilson line in N $$ \mathcalN} $$ = 4 SYM

Single particle operators and their correlators in free N $$ \mathcalN} $$ = 4 SYM

Spatially modulated and supersymmetric mass deformations of N $$ \mathcalN} $$ = 4 SYM

Supersymmetric phases of 4d N $$ \mathcalN} $$ = 4 SYM at large N

Integrated correlators in N $$ \mathcalN} $$ = 4 SYM via SL(2, ℤ) spectral theory

Four-point correlators in N $$ \mathcalN} $$ = 4 SYM from AdS5 bubbling geometries

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