The task of quantization consists of forming a quantum mechanical system fr
om a given classical system. Thereby, classical observables are replaced by
quantum mechanical observables. We carry out this procedure with Gibbs' ca
nonical ensemble. Therefrom, we obtain a density matrix which represents a
quantum mechanical concept of equipartition. The most important justificati
on for this principle is provided by the virial theorem. Thereafter, the im
plications of the density matrix are evaluated. For this purpose, we define
a virtual free energy. Thus, the equilibrium condition of the quantum cano
nical ensemble is derived by minimizing the virtual free energy. We demonst
rate our method for the case of a mean field like order-disorder phase tran
sition. This theory leads to new predictions for solids at low temperatures
. The model may, for instance, be applied to potassium dihydrogen phosphate
or its isomorphous compounds. (C) 2000 Elsevier Science B.V. All rights re
served.