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

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: 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

Creator: Bianchi, Massimo
Bossard, Guillaume
Consoli, Dario

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP06(2022)088

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

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

Last update: 15.08.2025, 7:35 AM CEST

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

Other Objects (12)

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

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

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

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

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

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

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

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

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

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

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

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$

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

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

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

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

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$

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

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

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

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

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

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

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

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

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

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

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

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

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$

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

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

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

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

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$

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

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

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

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

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

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

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

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

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

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

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

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

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$

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

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

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

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

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$

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

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

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Other Objects (12)

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

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

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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