We classify the local bifurcations of one dov quantum billiards, showing th
at only saddle-center bifurcations can occur. We analyze the resulting plan
ar system when there is no coupling in the superposition state. In so doing
, we also consider the global bifurcation structure. Using a double-well po
tential as a representative example, we demonstrate how to locate bifurcati
ons in parameter space. We also discuss how to approximate the cuspidal loo
p using AUTO as well as how to cross it via continuation by detuning the dy
namical system. Moreover, we show that when there is coupling, the resultin
g five-dimensional system - though chaotic - has a similar underlying struc
ture. We verify numerically that both homoclinic orbits and cusps occur and
provide an outline of an analytical argument for the existence of such hom
oclinic orbits. Small perturbations of the system reveal homoclinic tangles
that typify chaotic behavior.