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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Pure N=2 $$ \mathcalN}=2 $$ super Yang-Mills and exact WKB ; volume:2015 ; number:8 ; day:31 ; month:8 ; year:2015 ; pages:1-43 ; date:8.2015
Journal of high energy physics ; 2015, Heft 8 (31.8.2015), 1-43, 8.2015

Classification: Physik

Creator: Kashani-Poor, Amir-Kian

Contributor: Troost, Jan
SpringerLink (Online service)

DOI: 10.1007/JHEP08(2015)160

URN: urn:nbn:de:101:1-2018082502241659663454

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:38 AM CEST

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Kashani-Poor, Amir-Kian
Troost, Jan
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$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

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

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

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

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

$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

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

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

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

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

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

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Other Objects (12)

$ \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

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

$ \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

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

$ \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

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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