The spherical quantum billiard with a time-varying radius, a(t), is conside
red. It is proved that only superposition states with components of common
rotational symmetry give rise to chaos. Examples of both nonchaotic and cha
otic states are described. In both cases, a Hamiltonian is derived in which
a and P are canonical coordinate and momentum, respectively. For the chaot
ic case, working in Bloch variables (x,y,z), equations describing the motio
n are derived. A potential function is introduced which gives bounded motio
n of a(t). Poincare maps of (a,P) at x=0 and the Bloch sphere projected ont
o the (x,y) plane at P=0 both reveal chaotic characteristics. (C) 2000 Amer
ican Institute of Physics. [S1054-1500(00)00602-9].