Exact WKB analysis of N $$ \mathcalN} $$ = 2 gauge theories

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Exact WKB analysis of N $$ \mathcalN} $$ = 2 gauge theories ; volume:2016 ; number:7 ; day:21 ; month:7 ; year:2016 ; pages:1-52 ; date:7.2016
Journal of high energy physics ; 2016, Heft 7 (21.7.2016), 1-52, 7.2016

Creator: Ashok, Sujay K.

Contributor: Jatkar, Dileep P.
John, Renjan R.
Raman, M.
Troost, Jan
SpringerLink (Online service)

DOI: 10.1007/JHEP07(2016)115

URN: urn:nbn:de:1111-201607252765

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:56 AM CEST

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Ashok, Sujay K.
Jatkar, Dileep P.
John, Renjan R.
Raman, M.
Troost, Jan
SpringerLink (Online service)

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

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

$Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization$

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$Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories$

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$$ \mathcalN} = 8 $ superspace constraints for three-dimensional gauge theories$

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$Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling$

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

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

$Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization$

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

$Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories$

Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories

$Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory$

Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory

$Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters$

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

$Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories$

Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories

$Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics$

Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics

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$Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters$

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$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

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

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

$Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling$

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

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

$Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization$

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

$Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories$

Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories

$Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory$

Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory

$Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters$

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

$Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories$

Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories

$Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics$

Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics

$$ \mathcalN} = 8 $ superspace constraints for three-dimensional gauge theories$

$ \mathcalN} = 8 $ superspace constraints for three-dimensional gauge theories

$Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters$

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

$Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory$

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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Exact WKB analysis of N $$ \mathcalN} $$ = 2 gauge theories

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Other Objects (12)

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

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories

Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories

Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics

$ \mathcalN} = 8 $ superspace constraints for three-dimensional gauge theories

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories

Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories

Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics

$ \mathcalN} = 8 $ superspace constraints for three-dimensional gauge theories

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

Classification of 5d N $$ \mathcalN} $$ = 1 gauge theories

Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

Sequential deconfinement in 3d N $$ \mathcalN} $$ = 2 gauge theories

Dark Matter in scalar Sp( N $$ \mathcalN} $$ ) gauge dynamics

$ \mathcalN} = 8 $ superspace constraints for three-dimensional gauge theories

Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters

Holographic duals of the N $$ \mathcalN} $$ = 1* gauge theory

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