Abstract
The solution of the quantum dynamical equation idTdt=HT, for the time-displacement operator T, is given, when the Hamiltonian H is a polynomial of the second degree in canonically conjugate variables, with arbitrary time-dependent coefficients. Heisenberg's equations of motion are then solved, and the general integral of Schrödinger's equation in coordinate space is expressed by the Green's function corresponding to T. An example is given.

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