We show that, in spite of a rather common opinion, quantum mechanics can be
represented as an approximation of classical statistical mechanics. The
approximation under consideration is based on the ordinary Taylor expansion of
physical variables. The quantum contribution is given by the term of the second
order. To escape technical difficulties, we start with the finite dimensional
quantum mechanics. In our approach quantum mechanics is an approximative
theory. It predicts statistical averages only with some precision. In
principle, there might be found deviations of averages calculated within the
quantum formalism from experimental averages (which are supposed to be equal to
classical averages given by our model).Comment: Talks at the conferences: "Quantum Theory: Reconsideration of
Foundations-3", Vaxjo, Sweden, June-2005; "Processes in Physics", Askloster,
Sweden, June-2005; "The nature of light: What is photon?", San-Diego,
August-2005; "Nonlinear Physics. Theory and Experiment", Lece, Italy,
July-200