Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: 1 Online-Ressource.

Language: Englisch

Bibliographic citation: Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills ; volume:2023 ; number:8 ; day:16 ; month:8 ; year:2023 ; pages:1-13 ; date:8.2023
Journal of high energy physics ; 2023, Heft 8 (16.8.2023), 1-13, 8.2023

Classification: Physik

Creator: Catterall, Simon
Giedt, Joel
Toga, Goksu Can

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2023)084

URN: urn:nbn:de:101:1-2024011608290554967825

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

Last update: 15.08.2025, 7:20 AM CEST

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Catterall, Simon
Giedt, Joel
Toga, Goksu Can
SpringerLink (Online service)

Other Objects (12)

$4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography$

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory$

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

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

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

$Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills$

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

$The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

$Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2$

N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2

$4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography$

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory$

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

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

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

$Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills$

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

$The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

$Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2$

N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2

$4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography$

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

$$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3$

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

$Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma$

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

$Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory$

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

$Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling$

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

$On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory$

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

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

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

$Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills$

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

$The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory$

The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

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

$Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2$

N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2

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Holography from lattice N $$ \mathcalN} $$ = 4 super Yang-Mills

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Other Objects (12)

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

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

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

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

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2

4d N=1/2d $$ \mathcalN}=1/2d $$ Yang-Mills duality in holography

$ \mathcalN} $ = 4 supersymmetric Yang-Mills theories in AdS3

Magnetising the N $$ \mathcalN} $$ = 4 Super Yang-Mills plasma

Regge trajectories in N $$ \mathcalN} $$ = 2 supersymmetric Yang-Mills theory

Lattice N $$ \mathcalN} $$ = 4 super Yang-Mills at strong coupling

On BPS strings in N $$ \mathcalN} $$ = 4 Yang-Mills theory

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

Yangian invariants and cluster adjacency in N $$ \mathcalN} $$ = 4 Yang-Mills

The coupling flow of N $$ \mathcalN} $$ = 4 super Yang-Mills theory

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

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

N $$ \mathcalN} $$ = 4 supersymmetric Yang-Mills thermodynamics to order λ 2

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