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

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 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

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

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP08(2022)199

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

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

Last update: 17.08.8025, 4:43 AM CEST

Data provider

This object is provided by:
Deutsche Nationalbibliothek. If you have any questions about the object, please contact the data provider.

Show original at data provider

Associated

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

Other Objects (12)

$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

$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

Cultural heritage institutions wishing to register will find more information here.

Fields marked * need to be filled in.

Username*

Please enter your username

Email*

Please enter your email address

Please do not fill this field

First name

Last name

Password*

Please enter your password

Confirm password*

Please enter the same password

I have read the terms of use and the privacy policy for the collection of personal data and accept them. *

This field is required.

I would like to subscribe to the newsletter of the Deutsche Digitale Bibliothek. See newsletter subscription info.

Account created

Your "My DDB" account has been successfully created. Before you can log in to your account, you must click the confirmation link in the message we just sent to the email address you provided.

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

Object Details

References and Relationships

Contributors, Places and Time

Further information

Data provider

Associated

Other Objects (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

Related objects

Reset password