“…We assume that the dynamics of such a system is described by the quantum-classical Liouville equation 39,42,46,[55][56][57][58][59] . For a quantum operatorB W (X), which depends on the classical phase space variables X = (R, P ) = (R 1 , R 2 , ..., R N b , P 1 , P 2 , ..., P N b ) of the bath, this evolution equation takes the form,…”