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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Liouville theory, $ \mathcalN} = 2 $ gauge theories and accessory parameters ; volume:2012 ; number:5 ; day:9 ; month:5 ; year:2012 ; pages:1-26 ; date:5.2012
Journal of high energy physics ; 2012, Heft 5 (9.5.2012), 1-26, 5.2012

Creator: Ferrari, Franco
Piatek, Marcin

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP05(2012)025

URN: urn:nbn:de:101:1-2021080721241890339575

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

Last update: 14.08.2025, 10:51 AM CEST

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Ferrari, Franco
Piatek, Marcin
SpringerLink (Online service)

Other Objects (12)

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity$

N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

$N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions$

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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

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

$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

$4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups$

4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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

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

$Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories$

Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories

$Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories$

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity$

N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

$N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions$

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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

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

$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

$4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups$

4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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

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

$Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories$

Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories

$Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories$

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity$

N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

$N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions$

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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

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

$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

$4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups$

4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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

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

$Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories$

Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories

$Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories$

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

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

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Other Objects (12)

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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

4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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

Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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

4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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

Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

N = 2 $$ \mathcalN}=2 $$ supersymmetric gauge theories on S 2 × S 2 and Liouville Gravity

N = 1 $$ \mathcalN}=1 $$ Liouville SCFT in four dimensions

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

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

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

4d N $$ \mathcalN} $$ =2 theories with disconnected gauge groups

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

Strong coupling expansions in N $$ \mathcalN} $$ = 2 quiver gauge theories

Vertex Operator Algebras and 3d N $$ \mathcalN} $$ = 4 gauge theories

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