Bootstrapping the N $$ \mathcalN} $$ = 1 Wess-Zumino models in three dimensions

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Bootstrapping the N $$ \mathcalN} $$ = 1 Wess-Zumino models in three dimensions ; volume:2021 ; number:6 ; day:25 ; month:6 ; year:2021 ; pages:1-22 ; date:6.2021
Journal of high energy physics ; 2021, Heft 6 (25.6.2021), 1-22, 6.2021

Creator: Rong, Junchen
Su, Ning

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2021)153

URN: urn:nbn:de:101:1-2021121418521672874339

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

Last update: 15.08.2025, 7:38 AM CEST

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Rong, Junchen
Su, Ning
SpringerLink (Online service)

Other Objects (12)

$Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions$

Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions

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

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

$Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories$

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold$

Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD$

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

$N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions$

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions$

Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions

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

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

$Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories$

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold$

Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD$

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

$N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions$

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

$Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions$

Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions

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

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

$Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories$

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

$Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM$

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

$Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability$

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

$Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs$

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

$Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold$

Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold

$Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills$

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

$Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD$

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

$N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions$

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

$N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions$

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

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Bootstrapping the N $$ \mathcalN} $$ = 1 Wess-Zumino models in three dimensions

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Other Objects (12)

Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions

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

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions

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

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

Bootstrapping the minimal N $$ \mathcalN} $$ = 1 superconformal field theory in three dimensions

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

Bootstrapping line defects in N $$ \mathcalN} $$ : = 2 theories

Bootstrapping correlation functions in N = 4 $$ \mathcalN}=4 $$ SYM

Bootstrapping N $$ \mathcalN} $$ = 4 sYM correlators using integrability

Bootstrapping mixed correlators in 4D N $$ \mathcalN} $$ = 1 SCFTs

Bootstrapping mixed correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping N $$ \mathcalN} $$ = 4 super-Yang-Mills on the conformal manifold

Bootstrapping holographic defect correlators in N $$ \mathcalN} $$ = 4 super Yang-Mills

Bootstrapping 4d N $$ \mathcalN} $$ = 2 gauge theories: the case of SQCD

N $$ \mathcalN} $$ = 1 dualities in 2+1 dimensions

N $$ \mathcalN} $$ = 2 Liouville SCFT in four dimensions

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