We consider Aharonov-Bohm oscillations in a mesoscopic semiconductor r
ing threaded by both a constant magnetic flux and a time-dependent, re
sonant magnetic field with one or two frequencies. Working in the ball
istic regime, we establish that the theory of ''quantum nonlinear reso
nance'' applies, and thus that this system represents a possible solid
-state realization of ''quantum nonlinear resonance'' and ''quantum ch
aos.'' In particular, we investigate the behavior of the time-averaged
electron energy at zero temperature in the regimes of (i) an isolated
quantum nonlinear resonance and (ii) the transition to quantum chaos,
when two quantum nonlinear resonances overlap. The time-averaged ener
gy exhibits sharp resonant behavior as a function of the applied const
ant magnetic flux, and has a staircase dependence on the amplitude of
the external time-dependent field. In the chaotic regime, the resonant
behavior exhibits complex structure as a function of flux and frequen
cy. We compare and contrast the quantum chaos expected in these mesosc
opic ''solid-state atoms'' with that observed in Rydberg atoms in micr
owave fields, and discuss the prospects for experimental observation o
f the effects we predict.