Wall-crossing and operator ordering for ’t Hooft operators in N $$ \mathcalN} $$ = 2 gauge theories

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Wall-crossing and operator ordering for ’t Hooft operators in N $$ \mathcalN} $$ = 2 gauge theories ; volume:2019 ; number:11 ; day:21 ; month:11 ; year:2019 ; pages:1-53 ; date:11.2019
Journal of high energy physics ; 2019, Heft 11 (21.11.2019), 1-53, 11.2019

Creator: Hayashi, Hirotaka
Okuda, Takuya
Yoshida, Yutaka

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP11(2019)116

URN: urn:nbn:de:101:1-2020051723162775938042

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

Last update: 14.08.2025, 11:02 AM CEST

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Hayashi, Hirotaka
Okuda, Takuya
Yoshida, Yutaka
SpringerLink (Online service)

Other Objects (12)

ABCD of ’t Hooft operators

$Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories$

Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories

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

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

$Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

$Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories$

Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories

Q-operators are ’t Hooft lines

$Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs$

Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs

$The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators$

The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators

Urn models & operator ordering procedures

$Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD$

Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD

$Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories$

Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories

ABCD of ’t Hooft operators

$Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories$

Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories

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

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

$Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

$Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories$

Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories

Q-operators are ’t Hooft lines

$Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs$

Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs

$The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators$

The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators

Urn models & operator ordering procedures

$Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD$

Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD

$Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories$

Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories

ABCD of ’t Hooft operators

$Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories$

Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories

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

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

$Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories$

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

$Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories$

Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories

Q-operators are ’t Hooft lines

$Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs$

Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs

$The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators$

The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators

Urn models & operator ordering procedures

$Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD$

Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD

$Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories$

Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories

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Wall-crossing and operator ordering for ’t Hooft operators in N $$ \mathcalN} $$ = 2 gauge theories

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Other Objects (12)

ABCD of ’t Hooft operators

Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories

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

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories

Q-operators are ’t Hooft lines

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs

The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators

Urn models & operator ordering procedures

Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD

Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories

ABCD of ’t Hooft operators

Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories

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

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories

Q-operators are ’t Hooft lines

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs

The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators

Urn models & operator ordering procedures

Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD

Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories

ABCD of ’t Hooft operators

Loop operators in three-dimensional N $$ \mathcalN} $$ = 2 fishnet theories

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

Semi-chiral operators in 4d N $$ \mathcalN} $$ = 1 gauge theories

Seifert fibering operators in 3d N = 2 $$ \mathcalN}=2 $$ theories

Q-operators are ’t Hooft lines

Rebooting quarter-BPS operators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Spin 2 operators in holographic 4d N = 2 $$ \mathcalN}=2 $$ SCFTs

The most general 4 D $$ \mathcalD} $$ N $$ \mathcalN} $$ = 1 superconformal blocks for scalar operators

Urn models & operator ordering procedures

Modular properties of surface operators in N $$ \mathcalN} $$ = 2 SU(2) SQCD

Surface operators, chiral rings and localization in N $$ \mathcalN} $$ =2 gauge theories

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