Strong coupling expansion of free energy and BPS Wilson loop in N $$ \mathcalN} $$ = 2 superconformal models with fundamental hypermultiplets

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Strong coupling expansion of free energy and BPS Wilson loop in N $$ \mathcalN} $$ = 2 superconformal models with fundamental hypermultiplets ; volume:2021 ; number:8 ; day:20 ; month:8 ; year:2021 ; pages:1-42 ; date:8.2021
Journal of high energy physics ; 2021, Heft 8 (20.8.2021), 1-42, 8.2021

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

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2021)102

URN: urn:nbn:de:101:1-2021110817442472601683

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

Last update: 15.08.2025, 7:37 AM CEST

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

Other Objects (12)

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

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

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

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

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

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

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

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

$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

$BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories$

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM 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

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

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

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

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

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

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

$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

$BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories$

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM 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

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

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

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

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

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

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

$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

$BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories$

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

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Strong coupling expansion of free energy and BPS Wilson loop in N $$ \mathcalN} $$ = 2 superconformal models with fundamental hypermultiplets

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Other Objects (12)

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

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

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

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

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

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

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

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

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

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

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

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

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

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

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

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

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

BPS wilson loops in generic conformal N $$ \mathcalN} $$ = 2 SU(N) SYM theories

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