“…Therefore, a HJ theory finds solutions on the lower dimensional manifold Q and retrieves them on the higher dimensional manifold T * Q by the existence of a section γ of the cotangent bundle which is the solution γ of the Hamilton-Jacobi equation (1). This picture (3) can be devised in different situations, as it is the case of nonholonomic systems [14,23,32,37,39,50,51], geometric mechanics on Lie algebroids [5] and almost-Poisson manifolds, singular systems [41], Nambu-Poisson framework [44], control theory [7], classical field theories [38,40,45], partial differential equations in general [64], the geometric discretization of the Hamilton-Jacobi equation [43,52], and others [6,13].…”