Abstract

The quantum kicked rotor (QKR) map is embedded into a continuous unitary transformation generated by a time-independent quasi-Hamiltonian. In some vicinity of a quantum resonance of order qq, we relate the problem to the {\it regular} motion along a circle in a (q2−1)(q^2-1)-component inhomogeneous "magnetic" field of a quantum particle with qq intrinsic degrees of freedom described by the SU(q)SU(q) group. This motion is in parallel with the classical phase oscillations near a non-linear resonance.

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