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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters ; volume:2018 ; number:5 ; day:3 ; month:5 ; year:2018 ; pages:1-30 ; date:5.2018
Journal of high energy physics ; 2018, Heft 5 (3.5.2018), 1-30, 5.2018

Classification: Physik

Creator: Nii, Keita

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2018)017

URN: urn:nbn:de:101:1-2018071420371450570050

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:31 AM CEST

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SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$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

$Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

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

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

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

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

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

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

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

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

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

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

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

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

$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

$Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

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

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

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

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

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

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

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

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

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

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

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

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

$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

$Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

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

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

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

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

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

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

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

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

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

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Other Objects (12)

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

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

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

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

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

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

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

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

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

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

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

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

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

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

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

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

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

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

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

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

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

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