Abstract
A comoving reference frame in phase space is introduced in order to analyze the behaviour of time-dependent multi-dimensional quadratic. Hamiltonians. It is found that an explicit (time-dependent) representation exists in which the wave function always remains in a factorized form and independent of time. In this way the previous finding that the Wigner functions of such systems can be cast into factorized time-independent form by the introduction of appropriate time-dependent coordinates related to its integrals of motion is explained.
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