The superconformal index of class $ \mathcalS} $ theories of type D

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The superconformal index of class $ \mathcalS} $ theories of type D ; volume:2014 ; number:5 ; day:26 ; month:5 ; year:2014 ; pages:1-33 ; date:5.2014
Journal of high energy physics ; 2014, Heft 5 (26.5.2014), 1-33, 5.2014

Classification: Physik

Creator: Lemos, Madalena

Contributor: Peelaers, Wolfger
Rastelli, Leonardo
SpringerLink (Online service)

DOI: 10.1007/JHEP05(2014)120

URN: urn:nbn:de:1111-201801196916

Rights: Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:55 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

Lemos, Madalena
Peelaers, Wolfger
Rastelli, Leonardo
SpringerLink (Online service)

Other Objects (12)

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

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

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

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

$Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories$

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

$The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories$

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

$The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories$

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

Deformations of superconformal theories

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

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

$Chiral theories of class S $$ \mathcalS} $$$

Chiral theories of class S $$ \mathcalS} $$

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

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

$Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories$

Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories

$Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description$

Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

$Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories$

Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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

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

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

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

$Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories$

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

$The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories$

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

$The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories$

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

Deformations of superconformal theories

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

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

$Chiral theories of class S $$ \mathcalS} $$$

Chiral theories of class S $$ \mathcalS} $$

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

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

$Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories$

Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories

$Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description$

Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

$Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories$

Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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

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

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

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

$Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories$

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

$The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories$

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

$The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories$

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

Deformations of superconformal theories

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

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

$Chiral theories of class S $$ \mathcalS} $$$

Chiral theories of class S $$ \mathcalS} $$

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

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

$Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories$

Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories

$Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description$

Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

$Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories$

Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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.

The superconformal index of class $ \mathcalS} $ theories of type D

Object Details

References and Relationships

Classification and Topics

Contributors, Places and Time

Further information

Data provider

Associated

Other Objects (12)

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

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

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

Deformations of superconformal theories

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

Chiral theories of class S $$ \mathcalS} $$

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

Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories

Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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

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

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

Deformations of superconformal theories

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

Chiral theories of class S $$ \mathcalS} $$

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

Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories

Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

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

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

Superconformal indices of N $$ \mathcalN} $$ = 4 Chern-Simons matter theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

Deformations of superconformal theories

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

Chiral theories of class S $$ \mathcalS} $$

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

Universality of Toda equation in N = 2 $$ \mathcalN}=2 $$ superconformal field theories

Gravity duals of $ \mathcalN} $ = 2 superconformal field theories with no electrostatic description

Complete prepotential for 5d N $$ \mathcalN} $$ = 1 superconformal field theories

Related objects

Reset password