  Any time-dependent solution of Schr\"{o}dinger equation may be always
correlated to a solution of Hamilton equations or to a statistical combination
of their solutions; only the set of corresponding solutions is somewhat smaller
(due to existence of quantization). There is not any reason to the physical
interpretation according to Copenhagen alternative as Bell's inequalities are
valid in the classical physics only (and not in any alternative based on
Schr\"{o}dinger equation). The advantage of Schr\"{o}dinger equation consists
then in that it enables to represent directly the time evolution of a
statistical distribution of classical initial states (which is usual in
collision experiments). The Schr\"{o}dinger equation (without assumptions added
by Bohr) may then represent the common physical theory for microscopic as well
as macroscopic physical systems. However, together with the last possibility
the solutions of Schr\"{o}dinger equation may be helpful also in analyzing the
influence of other statistically distributed properties (e.g., spin
orientations or space structures) of individual matter objects forming a
corresponding physical system, which goes in principle beyond the classical
physics. In any case, the contemporary quantum theory represents the
phenomenological approximative description of some matter characteristics only,
without providing any insight into quantum mechanism emergence. In such a case
it is necessary to take into account more detailed properties at least of some
involved objects.
