Defect CFT techniques in the 6d N $$ \mathcalN} $$ = (2, 0) theory

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: Defect CFT techniques in the 6d N $$ \mathcalN} $$ = (2, 0) theory ; volume:2021 ; number:3 ; day:29 ; month:3 ; year:2021 ; pages:1-38 ; date:3.2021
Journal of high energy physics ; 2021, Heft 3 (29.3.2021), 1-38, 3.2021

Urheber: Drukker, Nadav
Probst, Malte
Trépanier, Maxime

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2021)261

URN: urn:nbn:de:101:1-2021052519294832133821

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

Letzte Aktualisierung: 14.08.2025, 11:02 MESZ

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Beteiligte

Drukker, Nadav
Probst, Malte
Trépanier, Maxime
SpringerLink (Online service)

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$Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape$

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$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

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$N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT$

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$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

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$Exact correlators on the Wilson loop in N=4 $$ \mathcalN}=4 $$ SYM: localization, defect CFT, and integrability$

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$Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape$

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$4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)$

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$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

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$Exact $$ \mathcalN} $$ = 2* Schur line defect correlators$

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$Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT$

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$Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape$

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$Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry$

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$N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT$

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Defect CFT techniques in the 6d N $$ \mathcalN} $$ = (2, 0) theory

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

Non-supersymmetric Wilson loop in N $$ \mathcalN} $$ = 4 SYM and defect 1d CFT

Unifying the 6D N $$ \mathcalN} $$ = (1, 1) string landscape

4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

N $$ \mathcalN} $$ = 4 superconformal bootstrap of the K3 CFT

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

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

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4d N = 1 $$ \mathcalN}=1 $$ from 6d (1, 0)

Stringy CFT duals with N $$ \mathcalN} $$ = (2, 2) supersymmetry

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Exact $$ \mathcalN} $$ = 2* Schur line defect correlators

Exact correlators on the Wilson loop in N=4 $$ \mathcalN}=4 $$ SYM: localization, defect CFT, and integrability

One-loop divergences in 6D, N $$ \mathcalN} $$ = (1, 0) SYM theory

Erratum to: Exact correlators on the Wilson loop in N $$ \mathcalN} $$ = 4 SYM: localization, defect CFT, and integrability

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