BPS Wilson loop in N $$ \mathcalN} $$ = 2 superconformal SU(N) “orientifold” gauge theory and weak-strong coupling interpolation

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: BPS Wilson loop in N $$ \mathcalN} $$ = 2 superconformal SU(N) “orientifold” gauge theory and weak-strong coupling interpolation ; volume:2021 ; number:7 ; day:14 ; month:7 ; year:2021 ; pages:1-30 ; date:7.2021
Journal of high energy physics ; 2021, Heft 7 (14.7.2021), 1-30, 7.2021

Creator: Beccaria, M.
Dunne, G. V.
Tseytlin, A. A.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP07(2021)085

URN: urn:nbn:de:101:1-2021101722574628279117

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

Last update: 15.08.2025, 7:34 AM CEST

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Beccaria, M.
Dunne, G. V.
Tseytlin, A. A.
SpringerLink (Online service)

Other Objects (12)

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

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

$BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories$

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

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

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

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

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

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

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

$BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories$

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

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

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

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

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

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

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

$BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories$

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

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

$The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap$

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

$Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks$

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

$Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers$

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

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

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

$Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory$

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

$Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

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

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

$Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers$

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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BPS Wilson loop in N $$ \mathcalN} $$ = 2 superconformal SU(N) “orientifold” gauge theory and weak-strong coupling interpolation

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Other Objects (12)

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

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

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

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

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

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

BPS Wilson loops in N $$ \mathcalN} $$ ≥ 2 superconformal Chern-Simons-matter theories

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

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Four-dimensional $$\mathcalN}$$ = 2 superconformal long circular quivers

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

Towards N $$ \mathcalN} $$ = 2 superconformal higher-spin theory

Chiral correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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

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

Wilson loop correlators in N $$ \mathcalN} $$ = 2 superconformal quivers

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