  We compute the conserved charges associated with the asymptotic symmetries of
massless particles by examining their free theory in Minkowski spacetime. We
give a procedure to systematically deduce the fall off of the massless fields
at spatial infinity and show that it has a universal behaviour when expressed
in tangent space. We do this for generic massless particles. We do not impose
gauge fixing conditions which allows us to uncover new nonzero charges for the
graviton beyond the well-known supertranslation charges. We also compute
conserved charges in the dual formulations of certain low spin particles and
argue that this leads to an infinite number of new conserved charges.

High Energy Physics - Theory