Except for problems with a single degree of freedom (or with only spin degree of freedom), one always has PDEs, not ODEs (or ODEs in function spaces, which is the former in disguise).
In nonrelativistic quantum mechanics based on wave functions you
always have the Schroedinger equation, just with different Hamiltonians. The conservative case has a selfadjoint ##H## (in the PT symmetric case with respect to a nonstandard inner product), the dissipative case typically has an optical potential. There are also potentials derived by complex scaling (N. Moiseyev, Quantum theory of resonances: calculating energies, widths and cross-sections by complex scaling,
Physics Reports 302.5-6 (1998): 212-293.)
But the dissipative case is often better modeled by using density operators/matrices, then the dynamics is that of a
Lindblad equation.