2016
DOI: 10.1016/j.nuclphysb.2016.04.022
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Fermionic higher-spin triplets in AdS

Abstract: We derive a metric-like Lagrangian and equations of motion, in AdS space, for multiplets of fermionic fields with spin ranged from 1/2 to s, from their frame-like formulation.Comment: 1+13 pages, v3: typos corrected, references adde

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Cited by 8 publications
(9 citation statements)
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“…5 It is worth pointing out that the Fang-Fronsdal action for a massless spin-(s + 1 2 ) field [13] is also described in terms of a triplet of fermionic gauge fields, Ψ α(s+1)α(s) , Ψ α(s−1)α(s) and Ψ α(s−1)α(s−2) and their conjugates, if one makes use of the two-component spinor notation, see section 6.9 of [44]. More generally, there exist bosonic and fermionic higher-spin triplet models in higher dimensions [45,46,47,48,49]. On-shell supersymmetric formulations for the generalised triplets in diverse dimensions have recently been given in [50].…”
Section: Massive Higher-spin Actions In Ads Spacementioning
confidence: 99%
See 1 more Smart Citation
“…5 It is worth pointing out that the Fang-Fronsdal action for a massless spin-(s + 1 2 ) field [13] is also described in terms of a triplet of fermionic gauge fields, Ψ α(s+1)α(s) , Ψ α(s−1)α(s) and Ψ α(s−1)α(s−2) and their conjugates, if one makes use of the two-component spinor notation, see section 6.9 of [44]. More generally, there exist bosonic and fermionic higher-spin triplet models in higher dimensions [45,46,47,48,49]. On-shell supersymmetric formulations for the generalised triplets in diverse dimensions have recently been given in [50].…”
Section: Massive Higher-spin Actions In Ads Spacementioning
confidence: 99%
“…where the Lagrangian L is a scalar superfield. In accordance with the general formalism described in section 6.4 of [44], the isometry transformations of AdS 3|2 are generated by the Killing vector fields ξ A E A which are defined to obey the master equation [65] ξ 49) for some Lorentz superfield parameter Λ bc = −Λ cb . An infinitesimal isometry transformation acts on a tensor superfield T as…”
Section: From Ads Superspace To Ads Spacementioning
confidence: 99%
“…Let us impose all the differential constraints via BRST operator, while all the algebraic constraints or, more precisely, their appropriate BRST invariant extensions we impose directly in the representation space. In the case of integer spin fields, this reproduces [28,48] the triplet formulation discussed previously in [49][50][51][52][53][54]. As we are going to see for half-integer spin fields this gives the extended description from which the familiar triplet formulation of [50,51] can be obtained by eliminating auxiliary fields and solving constraints.…”
Section: Extended Triplet Formulationmentioning
confidence: 60%
“…In Minkowski superspace, the action (4.28a) simplifies into In the bosonic sector, we have the following set of fields: The component structure of the obtained supermultiplets is a three-dimensional counterpart of so-called (reducible) higher-spin triplet systems. In AdS D an action for bosonic higher-spin triplets was constructed in [66] and for fermionic triplets in [67,68]. Our superfield construction provides a manifestly off-shell supersymmetric generalisation of these systems.…”
Section: B2 Massless Superspin-(s + 1 2 ) Actionmentioning
confidence: 99%