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The covariant description of massless particles of arbitrary spin typically employs symmetric tensors of rank and rests on a local symmetry carried by symmetric tensor parameters of rank , suitably generalizing the transformations of Maxwell’s theory and the diffeomorphisms underlying general relativity. Here we show that Fronsdal’s action is actually uniquely identified by the weaker requirement of invariance under higher-derivative gauge transformations driven by a vector parameter. This observation may hint to a tighter, if unexpected, connection between higher-spin symmetry and diffeomorphisms.

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