Symplectic geometry on the Hilbert phase space and foundations of quantum mechanics

We show that in the opposition to a rather common opinion quantum mechanics is not complete. It is possible to introduce so called hidden variable - in our model classical fields and combine the statistical predictions of quantum mechanics with deterministic dynamics of those bidden variables. Quantum mechanics can be considered as an approximative description of physical processes based on neglecting by quantities of the magnitude o(alpha), where alpha is the dispersion of fluctuations of the Gaussian background field. In this paper we present the detailed presentation of theory of infinite-dimensional phase space and derive main equations of quantum mechanics (e.g., Scbrodinger's equation, Heisenberg's equation and von Neumann equation) from the Hamilton equation on the infinite-dimensional symplectic space. We emphasize (to escape misunderstanding) that our paper is not about quantization of systems with infinite number of degrees of freedom, but about representation of quantum systems as classical systems with infinite number of degrees of freedom. We also investigate the purely mathematical problem of preserving of the dispersion of Gaussian fluctuations by Hamiltonian flows.