Holographic and localization calculations of boundary F for N $$ \mathcalN} $$ = 4 SUSY Yang-Mills theory

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Holographic and localization calculations of boundary F for N $$ \mathcalN} $$ = 4 SUSY Yang-Mills theory ; volume:2021 ; number:2 ; day:25 ; month:2 ; year:2021 ; pages:1-69 ; date:2.2021
Journal of high energy physics ; 2021, Heft 2 (25.2.2021), 1-69, 2.2021

Creator: Raamsdonk, Mark Van
Waddell, Chris

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2021)222

URN: urn:nbn:de:101:1-2021051614424236032269

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

Last update: 14.08.2025, 10:54 AM CEST

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Raamsdonk, Mark Van
Waddell, Chris
SpringerLink (Online service)

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

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$N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene$

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$Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds$

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

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

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Holographic and localization calculations of boundary F for N $$ \mathcalN} $$ = 4 SUSY Yang-Mills theory

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Other Objects (12)

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

Global symmetries and $$\mathcalN}=2$$ N = 2 SUSY

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

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

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

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

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

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

Global symmetries and $$\mathcalN}=2$$ N = 2 SUSY

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

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

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

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

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

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

Global symmetries and $$\mathcalN}=2$$ N = 2 SUSY

A holographic kaleidoscope for N $$ \mathcalN} $$ = 1*

Holographic 3d N $$ \mathcalN} $$ = 1 conformal manifolds

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

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

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

N $$ \mathcalN} $$ -extended D = 4 supergravity, unconventional SUSY and graphene

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

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

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

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

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