Confinement in 3d N $$ \mathcalN} $$ = 2 Spin(N) gauge theories with vector and spinor matters

to related objects

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Confinement in 3d N $$ \mathcalN} $$ = 2 Spin(N) gauge theories with vector and spinor matters ; volume:2019 ; number:3 ; day:20 ; month:3 ; year:2019 ; pages:1-31 ; date:3.2019
Journal of high energy physics ; 2019, Heft 3 (20.3.2019), 1-31, 3.2019

Creator: Nii, Keita

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2019)113

URN: urn:nbn:de:101:1-2019050121003521196843

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

Last update: 14.08.2025, 10:49 AM CEST

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Other Objects (12)

$Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

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

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

$Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters$

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

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

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

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

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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

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

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

$Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters$

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

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

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

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

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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

$Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory$

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

$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

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

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

$Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters$

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

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

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

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

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

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

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

$4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)$

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

$N $$ \mathcalN} $$ = 2* Schur indices$

N $$ \mathcalN} $$ = 2* Schur indices

$N $$ \mathcalN} $$ = 1 conformal dualities$

N $$ \mathcalN} $$ = 1 conformal dualities

$Liberated N $$ \mathcalN} $$ = 1 supergravity$

Liberated N $$ \mathcalN} $$ = 1 supergravity

$N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs$

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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Confinement in 3d N $$ \mathcalN} $$ = 2 Spin(N) gauge theories with vector and spinor matters

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Other Objects (12)

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

N $$ \mathcalN} $$ = 2* Schur indices

N $$ \mathcalN} $$ = 1 conformal dualities

Liberated N $$ \mathcalN} $$ = 1 supergravity

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

N $$ \mathcalN} $$ = 2* Schur indices

N $$ \mathcalN} $$ = 1 conformal dualities

Liberated N $$ \mathcalN} $$ = 1 supergravity

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

Correlation functions of spinor current multiplets in N $$ \mathcalN} $$ = 1 superconformal theory

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

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

Exact results in 3d N $$ \mathcalN} $$ = 2 Spin(7) gauge theories with vector and spinor matters

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

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

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

4d N $$ \mathcalN} $$ : = 1 from 6d D-type N $$ \mathcalN} $$ = (1, 0)

N $$ \mathcalN} $$ = 2* Schur indices

N $$ \mathcalN} $$ = 1 conformal dualities

Liberated N $$ \mathcalN} $$ = 1 supergravity

N = 1 $$ \mathcalN}=1 $$ deformations and RG flows of N = 2 $$ \mathcalN}=2 $$ SCFTs

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