Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories ; volume:2020 ; number:2 ; day:12 ; month:2 ; year:2020 ; pages:1-71 ; date:2.2020
Journal of high energy physics ; 2020, Heft 2 (12.2.2020), 1-71, 2.2020

Creator: Hayashi, Hirotaka
Kim, Sung-Soo
Lee, Kimyeong
Yagi, Futoshi

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP02(2020)074

URN: urn:nbn:de:101:1-2020051120461573514942

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

Last update: 14.08.2025, 10:59 AM CEST

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Hayashi, Hirotaka
Kim, Sung-Soo
Lee, Kimyeong
Yagi, Futoshi
SpringerLink (Online service)

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$Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories$

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$BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories$

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Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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Other Objects (12)

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

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

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

Probing N = 2 $$ \mathcalN}=2 $$ superconformal field theories with localization

S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

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

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

Probing N = 2 $$ \mathcalN}=2 $$ superconformal field theories with localization

S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

Reviving 3D N $$ \mathcalN} $$ = 8 superconformal field theories

Mixed OPEs in N = 2 $$ \mathcalN}=2 $$ superconformal theories

New N $$ \mathcalN} $$ = 2 superconformal field theories from S $$ \mathcalS} $$ -folds

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

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

Probing N = 2 $$ \mathcalN}=2 $$ superconformal field theories with localization

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The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

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