We study the effect of a strong electron-electron (e-e) interaction in
a system of two concentric one-dimensional rings with incommensurate
areas A(1) and A(2), coupled by a tunnel amplitude. For noninteracting
particles the magnetic moment (persistent current) m of the many-body
ground state and first excited states is an irregular function of the
external magnetic field. In contrast, we show that when strong e-e in
teractions are present the magnetic-field dependence of m becomes peri
odic. In such a strongly correlated system disorder can only be caused
by inter-ring charge fluctuations, controllable by a gate voltage. Th
e oscillation period of m is proportional to 1/(A(1) + A(2)) if fluctu
ations are suppressed. Coherent inter-ring tunneling doubles the perio
d when charge fluctuations are allowed.