The operator product expansions in the $$\mathcalN}=4$$ N=4 orthogonal Wolf space coset model

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1434-6052

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The operator product expansions in the $$\mathcalN}=4$$ N=4 orthogonal Wolf space coset model ; volume:79 ; number:7 ; day:10 ; month:7 ; year:2019 ; pages:1-24 ; date:7.2019
The European physical journal / C. C, Particles and fields ; 79, Heft 7 (10.7.2019), 1-24, 7.2019

Creator: Ahn, Changhyun
Kim, Man Hea
Paeng, Jinsub

Contributor: SpringerLink (Online service)

DOI: 10.1140/epjc/s10052-019-7091-y

URN: urn:nbn:de:101:1-2020012121352542162044

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

Last update: 14.08.2025, 10:47 AM CEST

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Ahn, Changhyun
Kim, Man Hea
Paeng, Jinsub
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$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

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

$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

$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

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

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

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

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

$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

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

$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

$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

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

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

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

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

$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

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

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

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

$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

$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

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The operator product expansions in the $$\mathcalN}=4$$ N=4 orthogonal Wolf space coset model

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Other Objects (12)

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

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

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

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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

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

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

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

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

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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

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

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

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

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

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

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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

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

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