The notion that conserved quantities (or quantities for which there is something like a continuity equation) correspond to symmetries of the action of a physical system can be formulated in various different realms (classical mechanics, field theory, Lagrangian / Hamiltonian formalism, QM, QFT ...). When it is formulated in QFT / QM we usually employ the operator formalism, and see that operators that commute with the Hamiltonian generate transformations that are symmetries.
I'd like to know if there is similar thing in the path integral formulation of quantum mechanics (which essentially doesn't know any operators).