Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

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Standort: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Umfang: Online-Ressource

Sprache: Englisch

Anmerkungen: online resource.

Erschienen in: Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds ; volume:2022 ; number:6 ; day:15 ; month:6 ; year:2022 ; pages:1-96 ; date:6.2022
Journal of high energy physics ; 2022, Heft 6 (15.6.2022), 1-96, 6.2022

Urheber: Bianchi, Massimo
Bossard, Guillaume
Consoli, Dario

Beteiligte Personen und Organisationen: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2022)088

URN: urn:nbn:de:101:1-2022081621510863833687

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

Letzte Aktualisierung: 15.08.2025, 07:35 MESZ

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Beteiligte

Bianchi, Massimo
Bossard, Guillaume
Consoli, Dario
SpringerLink (Online service)

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$Superfield approach to higher derivative N $$ \mathcalN} $$ = 1 superconformal mechanics$

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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

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Perturbative higher-derivative terms in N $$ \mathcalN} $$ = 6 asymmetric orbifolds

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Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

Exact moduli spaces for N $$ \mathcalN} $$ = 2, D = 5 freely acting orbifolds

Superfield approach to higher derivative N $$ \mathcalN} $$ = 1 superconformal mechanics

Perturbative solutions of N = 1 ∗ $$ \mathcalN}={1}^{\ast } $$ holography on S 4

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

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

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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

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

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

Large N non-perturbative effects in N = 4 $$ \mathcalN}=4 $$ superconformal Chern-Simons theories

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

Non-perturbative geometries for planar N $$ \mathcalN} $$ = 4 SYM amplitudes

New quantum toroidal algebras from 5D N $$ \mathcalN} $$ = 1 instantons on orbifolds

N $$ \mathcalN} $$ =2 heterotic string compactifications on orbifolds of K3 × T 2

Exact moduli spaces for N $$ \mathcalN} $$ = 2, D = 5 freely acting orbifolds

Superfield approach to higher derivative N $$ \mathcalN} $$ = 1 superconformal mechanics

Perturbative solutions of N = 1 ∗ $$ \mathcalN}={1}^{\ast } $$ holography on S 4

Perturbative four-point functions in planar N = 4 $$ \mathcalN}=4 $$ SYM From hexagonalization

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

Large N non-perturbative effects in N = 4 $$ \mathcalN}=4 $$ superconformal Chern-Simons theories

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

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