Cubic interactions for arbitrary spin N $$ \mathcalN} $$ -extended massless supermultiplets in 4d flat space

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Cubic interactions for arbitrary spin N $$ \mathcalN} $$ -extended massless supermultiplets in 4d flat space ; volume:2019 ; number:11 ; day:14 ; month:11 ; year:2019 ; pages:1-32 ; date:11.2019
Journal of high energy physics ; 2019, Heft 11 (14.11.2019), 1-32, 11.2019

Creator: Metsaev, R.R

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP11(2019)084

URN: urn:nbn:de:101:1-2020051723171276392960

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

Last update: 14.08.2025, 10:51 AM CEST

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Metsaev, R.R
SpringerLink (Online service)

Other Objects (12)

Cubic interaction vertices for massive/massless continuous-spin fields and arbitrary spin fields

Cubic interaction vertices for N=1 arbitrary spin massless supermultiplets in flat space

Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions

$N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations$

N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations

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

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

Massless Lifshitz field theory for arbitrary z

$Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields$

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

$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

Cubic interactions for massless and partially massless spin-1 and spin-2 fields

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

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

Cubic interaction vertices for massive/massless continuous-spin fields and arbitrary spin fields

Cubic interaction vertices for N=1 arbitrary spin massless supermultiplets in flat space

Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions

$N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations$

N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations

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

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

Massless Lifshitz field theory for arbitrary z

$Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields$

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

$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

Cubic interactions for massless and partially massless spin-1 and spin-2 fields

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

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

Cubic interaction vertices for massive/massless continuous-spin fields and arbitrary spin fields

Cubic interaction vertices for N=1 arbitrary spin massless supermultiplets in flat space

Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions

$N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations$

N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations

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

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

Massless Lifshitz field theory for arbitrary z

$Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields$

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

$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

Cubic interactions for massless and partially massless spin-1 and spin-2 fields

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

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

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Cubic interactions for arbitrary spin N $$ \mathcalN} $$ -extended massless supermultiplets in 4d flat space

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Other Objects (12)

Cubic interaction vertices for massive/massless continuous-spin fields and arbitrary spin fields

Cubic interaction vertices for N=1 arbitrary spin massless supermultiplets in flat space

Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions

N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations

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

Massless Lifshitz field theory for arbitrary z

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

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

Cubic interactions for massless and partially massless spin-1 and spin-2 fields

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

Cubic interaction vertices for massive/massless continuous-spin fields and arbitrary spin fields

Cubic interaction vertices for N=1 arbitrary spin massless supermultiplets in flat space

Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions

N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations

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

Massless Lifshitz field theory for arbitrary z

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

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

Cubic interactions for massless and partially massless spin-1 and spin-2 fields

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

Cubic interaction vertices for massive/massless continuous-spin fields and arbitrary spin fields

Cubic interaction vertices for N=1 arbitrary spin massless supermultiplets in flat space

Conserved higher spin supercurrents for arbitrary spin massless supermultiplets and higher spin superfield cubic interactions

N $$ \mathcalN} $$ = 2 supersymmetric partially massless fields and other exotic non-unitary superconformal representations

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

Massless Lifshitz field theory for arbitrary z

Off-shell cubic hypermultiplet couplings to N $$ \mathcalN} $$ = 2 higher spin gauge superfields

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

Cubic interactions for massless and partially massless spin-1 and spin-2 fields

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

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