“…The comparison between the determining equations for the Lie point infinitesimal symmetries of the PDE (10) and the determining equation for the stochastic symmetries for the SDE (9) arising in theorem 3.13 is not straightforward, first of all due to the different nature of the involved objects. Indeed, when we look for the infinitesimal symmetries of the PDE we look for a vector field of the form (12), while when we search symmetries for SDE (9), we deal with an infinitesimal transformation V = (Y, C, τ , H), where Y is a vector field on R n+1 , C : R n+1 → so(m), τ : R n+1 → R and H : R n+1 → R m are smooth functions.…”