We study the fractal scattering patterns of collinear collisions betwe
en an electron and a helium ion or a hydrogen atom. We have found that
the collisional time plotted against initial energy or initial phase
consists of a bi-infinite sequence of cusp-shaped regular intervals in
terlaced by chaotic bands and repeated enlargements of the chaotic ban
ds show similar patterns. These patterns resemble the previous ones ob
tained in the retrograde region of the coplanar scattering system, how
ever, the dynamical origin of the self-similar patterns is different a
nd can be understood in terms of various combinations of motions perpe
ndicular and parallel to the Wannier ridge and binary collisions. In p
articular, we have found that the trajectories near the cusp tips of r
egular intervals are strongly influenced by a set of triple-collision
orbits, trajectories originate and end at the triple-collision point.
Using the code and winding number for these orbits, we can organize th
e fractal scattering patterns into a tree structure. Furthermore, usin
g an ensemble of trajectories with uniformly selected initial phases,
we calculate the transition probabilities of excited electronic states
from a certain initial state of the hydrogenlike ion or atom using th
e quasiclassical trajectory method. These transition probabilities ill
ustrate that chaotic regions on the average correspond to higher elect
ronic excitation than that corresponding to the regular regions.