Conformal interactions between matter and higher-spin (super)fields
arXiv:2208.07783 · doi:10.1002/prop.202200157
Abstract
In even spacetime dimensions, the interacting bosonic conformal higher-spin (CHS) theory can be realised as an induced action. The main ingredient in this definition is the model describing a complex scalar field coupled to an infinite set of background CHS fields , with possessing a non-abelian gauge symmetry. Two characteristic features of the perturbative constructions of given in the literature are: (i) the background spacetime is flat; and (ii) conformal invariance is not manifest. In the present paper we provide a new derivation of this action in four dimensions such that (i) is defined on an arbitrary conformally-flat background; and (ii) the background conformal symmetry is manifestly realised. Next, our results are extended to the supersymmetric case. Specifically, we construct, for the first time, a model for a conformal scalar/chiral multiplet coupled to an infinite set of background higher-spin superfields . Our action possesses a non-abelian gauge symmetry which naturally generalises the linearised gauge transformations of conformal half-integer superspin multiplets. The other fundamental features of this model are: (i) is defined on an arbitrary conformally-flat superspace background; and (ii) the background superconformal symmetry is manifest. Making use of , an interacting superconformal higher-spin theory can be defined as an induced action.
arXiv comment69 pages; V2: References and new comments added, typos corrected; V3: Published version
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