A study of N $$ \mathcalN} $$ = 1 SCFT derived from N $$ \mathcalN} $$ = 2 SCFT: index and chiral ring

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Location: Deutsche Nationalbibliothek Frankfurt am Main

Extent: Online-Ressource, 1 online resource.

Language: Englisch

Bibliographic citation: A study of N $$ \mathcalN} $$ = 1 SCFT derived from N $$ \mathcalN} $$ = 2 SCFT: index and chiral ring ; volume:2023 ; number:3 ; day:27 ; month:3 ; year:2023 ; pages:1-40 ; date:3.2023
Journal of high energy physics ; 2023, Heft 3 (27.3.2023), 1-40, 3.2023

Classification: Physik

Creator: Xie, Dan
Yan, Wenbin

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2023)201

URN: urn:nbn:de:101:1-2023092610111105262489

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

Last update: 24.08.2020, 1:00 AM CEST

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Xie, Dan
Yan, Wenbin
SpringerLink (Online service)

Other Objects (12)

$4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras$

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

$The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories$

The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories

$Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT$

Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow$

Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow

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

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

$W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes$

W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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

$4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras$

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

$The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories$

The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories

$Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT$

Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow$

Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow

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

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

$W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes$

W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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

$4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras$

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

$The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories$

The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories

$Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT$

Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT

$On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs$

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

$Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow$

Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow

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

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

$W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes$

W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes

$N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$$

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

$An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

$N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity$

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

$A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking$

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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

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A study of N $$ \mathcalN} $$ = 1 SCFT derived from N $$ \mathcalN} $$ = 2 SCFT: index and chiral ring

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Other Objects (12)

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories

Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow

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

W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories

Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow

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

W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

4d N $$ \mathcalN} $$ = 2 SCFTs and lisse W-algebras

The moduli space of vacua of N = 2 $$ \mathcalN}=2 $$ class S $$ \mathcalS} $$ theories

Three dimensional canonical singularity and five dimensional N $$ \mathcalN} $$ = 1 SCFT

On low rank 4d N $$ \mathcalN} $$ = 2 SCFTs

Semicontinuity of 4d N = 2 $$ \mathcalN}=2 $$ spectrum under renormalization group flow

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

W algebras, cosets and VOAs for 4d N $$ \mathcalN} $$ = 2 SCFTs from M5 branes

N $$ \mathcalN} $$ = 2 Conformal SYM theories at large N $$ \mathcalN} $$

An N $$ \mathcalN} $$ = 1 Lagrangian for an N $$ \mathcalN} $$ = 3 SCFT

N $$ \mathcalN} $$ = 2 CFT3’s from N $$ \mathcalN} $$ = 4 gauged supergravity

A superfield constraint for N $$ \mathcalN} $$ : = 2 → N $$ \mathcalN} $$ = 0 breaking

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

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