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

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Alternative title: 2 theories

Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Bootstrapping line defects in N $$ \mathcalN} $$ ; volume:2020 ; number:3 ; day:20 ; month:3 ; year:2020 ; pages:1-46 ; date:3.2020
Journal of high energy physics ; 2020, Heft 3 (20.3.2020), 1-46, 3.2020

Creator: Gimenez-Grau, Aleix
Liendo, Pedro

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2020)121

URN: urn:nbn:de:101:1-2020061321113875637780

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

Last update: 14.08.2025, 11:03 AM CEST

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Gimenez-Grau, Aleix
Liendo, Pedro
SpringerLink (Online service)

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

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

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

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

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

$Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories$

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ 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

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Bootstrapping line defects in Ν=2 theories

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

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

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

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

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

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

$Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories$

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ 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

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Bootstrapping line defects in Ν=2 theories

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

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

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

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

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

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

$Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ theories$

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ 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

$Exceptional N = 3 $$ \mathcalN}=3 $$ theories$

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Bootstrapping line defects in Ν=2 theories

$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

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

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Other Objects (12)

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

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

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

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ 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

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Bootstrapping line defects in Ν=2 theories

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

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

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

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ 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

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Bootstrapping line defects in Ν=2 theories

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

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

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

Duality walls and defects in 5d N = 1 $$ \mathcalN}=1 $$ 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

Exceptional N = 3 $$ \mathcalN}=3 $$ theories

Bootstrapping line defects in Ν=2 theories

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

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