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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Exact partition functions for the Ω-deformed N = 2 ∗ $$ \mathcalN}={2}^{\ast } $$ SU(2) gauge theory ; volume:2016 ; number:7 ; day:12 ; month:7 ; year:2016 ; pages:1-24 ; date:7.2016
Journal of high energy physics ; 2016, Heft 7 (12.7.2016), 1-24, 7.2016

Classification: Physik

Creator: Beccaria, Matteo

Contributor: Macorini, Guido
SpringerLink (Online service)

DOI: 10.1007/JHEP07(2016)066

URN: urn:nbn:de:101:1-2018071222251523605694

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:24 AM CEST

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Beccaria, Matteo
Macorini, Guido
SpringerLink (Online service)

Other Objects (12)

$Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours$

Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours

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

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

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality$

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

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

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

$Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories$

Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories

$Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets$

Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets

$Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory$

Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

$4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions$

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

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

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

$One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect$

One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours$

Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours

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

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

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality$

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

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

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

$Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories$

Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories

$Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets$

Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets

$Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory$

Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

$4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions$

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

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

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

$One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect$

One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours$

Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours

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

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

$Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets$

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

$Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality$

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

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

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

$Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories$

Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories

$Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets$

Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets

$Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory$

Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

$4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions$

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

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

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

$One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect$

One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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

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Other Objects (12)

Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours

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

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

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

Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories

Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets

Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

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

One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours

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

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

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

Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories

Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets

Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

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

One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

Exact partition functions for deformed N = 2 $$ \mathcalN}=2 $$ theories with N f = 4 $$ \mathcal{N}}_f=4 $$ flavours

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

Partial N $$ \mathcalN} $$ = 2 supersymmetry breaking and deformed hypermultiplets

Deformed $ \mathcalN}=2 $ theories, generalized recursion relations and S-duality

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

Chiral trace relations in Ω-deformed N = 2 $$ \mathcalN}=2 $$ theories

Deformed N=8 $$ \mathcalN}=8 $$ mechanics of (8, 8, 0) multiplets

Exact Holography and Black Hole Entropy in N = 8 $$ \mathcalN}=8 $$ and N = 4 $$ \mathcalN}=4 $$ String Theory

4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions

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

One-point functions in β-deformed N = 4 $$ \mathcalN}=4 $$ SYM with defect

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

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