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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 4d N $$ \mathcalN} $$ = 2 supergravity observables from Nekrasov-like partition functions ; volume:2022 ; number:2 ; day:10 ; month:2 ; year:2022 ; pages:1-56 ; date:2.2022
Journal of high energy physics ; 2022, Heft 2 (10.2.2022), 1-56, 2.2022

Creator: Hristov, Kiril

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2022)079

URN: urn:nbn:de:101:1-2022051721434505800871

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

Last update: 15.08.2025, 7:37 AM CEST

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Hristov, Kiril
SpringerLink (Online service)

Other Objects (12)

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions$

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

$Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity$

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions$

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

$Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity$

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity$

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

$Twistor strings for N $$ \mathcalN} $$ = 8 supergravity$

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

$Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity$

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

$N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models$

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

$Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling$

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

$N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions$

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

$Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity$

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

$Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity$

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

$N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions$

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

$Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity$

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

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

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Other Objects (12)

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

Liberated N $$ \mathcalN} $$ = 1 supergravity

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

Gauged D = 4 N $$ \mathcalN} $$ = 4 supergravity

Twistor strings for N $$ \mathcalN} $$ = 8 supergravity

Supersymmetric solitons in gauged N $$ \mathcalN} $$ = 8 supergravity

N $$ \mathcalN} $$ : = 2 JT supergravity and matrix models

Isometries, gaugings and N $$ \mathcalN} $$ = 2 supergravity decoupling

N $$ \mathcalN} $$ = 4 conformal supergravity: the complete actions

Swampland constraints on 5d N $$ \mathcalN} $$ = 1 supergravity

Minimal N = 4 $$ \mathcalN}=4 $$ topologically massive supergravity

N $$ \mathcalN} $$ = 2 conformal supergravity in five dimensions

Goldstino superfields in N = 2 $$ \mathcalN}=2 $$ supergravity

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