Three-point functions in a N $$ \mathcalN} $$ = 2 superconformal gauge theory and their strong-coupling limit

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: Three-point functions in a N $$ \mathcalN} $$ = 2 superconformal gauge theory and their strong-coupling limit ; volume:2022 ; number:8 ; day:19 ; month:8 ; year:2022 ; pages:1-39 ; date:8.2022
Journal of high energy physics ; 2022, Heft 8 (19.8.2022), 1-39, 8.2022

Urheber: Billò, M.
Frau, M.
Lerda, A.
Pini, A.
Vallarino, P.

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2022)199

URN: urn:nbn:de:101:1-2022110921011687446976

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

Letzte Aktualisierung: 15.08.2025, 07:38 MESZ

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Beteiligte

Billò, M.
Frau, M.
Lerda, A.
Pini, A.
Vallarino, P.
SpringerLink (Online service)

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$Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization$

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

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$R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories$

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

$Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

$Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling$

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

$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

$Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization$

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

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

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

$R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories$

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

$Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

$Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling$

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

$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

$Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization$

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

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

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

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Three-point functions in a N $$ \mathcalN} $$ = 2 superconformal gauge theory and their strong-coupling limit

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Ähnliche Objekte (12)

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

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

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

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

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

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

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

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

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

Three-point functions of higher-spin spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

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

Exact results in a N $$ \mathcalN} $$ = 2 superconformal gauge theory at strong coupling

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

Exact strong coupling results in N $$ \mathcalN} $$ = 2 Sp(2N) superconformal gauge theory from localization

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

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