  We show that the orbital Josephson effect appears in a wide range of driven
atomic Bose-Einstein condensed systems, including quantum ratchets, double
wells and box potentials. We use three separate numerical methods:
Gross-Pitaevskii equation, exact diagonalization of the few-mode problem, and
the Multi-Configurational Time-Dependent Hartree for Bosons algorithm. We
establish the limits of mean-field and few-mode descriptions, demonstrating
that they represent the full many-body dynamics to high accuracy in the weak
driving limit. Among other quantum measures, we compute the instantaneous
particle current and the occupation of natural orbitals. We explore four
separate dynamical regimes, the Rabi limit, chaos, the critical point, and
self-trapping; a favorable comparison is found even in the regimes of dynamical
instabilities or macroscopic quantum self-trapping. Finally, we present an
extension of the (t,t')-formalism to general time-periodic equations of motion,
which permits a systematic description of the long-time dynamics of resonantly
driven many-body systems, including those relevant to the orbital Josephson
effect.
