“…[79] In the position representation, the semiclassical propagator is a matrix whose elements are obtained as products of a complex action exponential and a stationary-phase pre-exponential factor, summed over all classical trajectories that connect the two endpoints. [41,[80][81][82][83][84][85][86][87][88] The search for these trajectories is hampered by the rigid double-boundary condition. In the SC-IVR dynamics, introduced by Miller and later also developed by Heller, Herman, Kluk, and Kay, [22,27,28,30,31,34,57,89] the propagator is instead formulated in terms of classical trajectories determined by initial condi-…”