We investigate, by numerical simulation, the path probability of non
dissipative mechanical systems undergoing stochastic motion. The aim is to
search for the relationship between this probability and the usual mechanical
action. The model of simulation is a one-dimensional particle subject to
conservative force and Gaussian random displacement. The probability that a
sample path between two fixed points is taken is computed from the number of
particles moving along this path, an output of the simulation, devided by the
total number of particles arriving at the final point. It is found that the
path probability decays exponentially with increasing action of the sample
paths. The decay rate increases with decreasing randomness. This result
supports the existence of a classical analog of the Feynman factor in the path
integral formulation of quantum mechanics for Hamiltonian systems.Comment: 19 pages, 6 figures, 1 table. It is a new text based on
arXiv:1202.0924 (to be withdrawn) with a completely different presentation.
Accepted by Chaos, Solitons & Fractals for publication 201