A semiclassical formula for the coherent-state propagator requires the dete
rmination of specific classical paths inhabiting a complex phase-space and
governed by a Hamiltonian flux. Such trajectories are constrained to specia
l boundary conditions which render their determination difficult by common
methods. In this paper we present a new method based on Runge-Kutta integra
tor for a quick, easy and accurate determination of these trajectories. Usi
ng nonlinear one dimensional systems we show that the semiclassical formula
is highly accurate as compared to its exact counterpart. Further, we clari
fy how the phase of the semiclassical approximation is correctly retrieved
during the time evolution.