“…Since the wall on the left has a height lower than the classical barrier for sufficiently large s, tunneling is possible when a quasiclassical trajectory crosses over the wall into the unbounded region to the left, where it will then continue almost freely except for one possible reflection at the U/s 2 potential. A detailed analysis of trajectories, given in [7], showed that the potential (2.17) does not reliably describe tunneling because the uniform nature of the channel, seen in figure 2, makes it much more likely for trajectories to follow the channel, rather than crossing the wall to the left. The fourth-order modification in (2.18), motivated by a more Gaussian behavior of states, was found to improve the tunneling description by quasiclassical trajectories.…”