Unconstrained Massless Higher Spin Supermultiplet in AdS${}_4$

We consider unconstrained formulation of the higher spin gauge theory in anti de Sitter (AdS) spacetime, given by actions [1, 2], and provide on-shell supersymmetry transformations for the $\mathcal{N}=1$ unconstrained massless higher spin supermultiplet in four-dimensional AdS${}_4$. Such an irreducible supermultiplet $({\mathrm{\Phi }}_1,{\mathrm{\Phi }}_2;{\mathrm{\Psi }}_1,{\mathrm{\Psi }}_2)$ contains a pair of bosonic fields, with opposite parity, which are generating functions (infinite collection of totally symmetric real tensor fields of all integer rank $s= 0, 1, \ldots, \infty$), as well as two fermionic fields, which have opposite signs of the AdS radius, that are spinorial generating functions (infinite tower of totally symmetric Majorana spinor-tensor fields of all half-integer spin $s=\frac{1}{2},\frac{3}{2},\dots ,\mathrm{\infty }$).