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Commun. math . Phys . 40, 153—174 (1975)
© by Springer-Verlag 1975
General Concept of Quantization
F. A. Berezin*
Academy of Sciences of the Ukrainian SSR, Institute for Theoretical Physics,
Kiev, Ukrainian, SSR
Received Jun e 15, 1974
Abstract. The general definition of quantization is proposed . As an example two
classical systems are considered. For the first of them the phase space is a Lobachevskii
plane, for the second one the two-dimensional sphere.
It is generally accepted that the quantization is an algorithm by
means of which a quantum system corresponds to a classical dynamic
one. Furthermore, it is required that in the limit ft-0 where h is the
Plancks constant, a quantum dynamic system change to a corresponding
classical one. This requirement is called the . correspondence principle.
It is quite obvious that there exist quite a lot quantizations obeying the
correspondence principle ; the quantum description of a physical
phenomenon is more detailed than the classical one, and so there are
certain phenomena the difference between which is displayed in their
quantum description, whereas their classical description does not show
this difference.
The following intuitive method of quantizing the classical dynamic
systems with a flat phase space has become well known since the
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