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Titlebook: Geometric Quantization and Quantum Mechanics; J?drzej ?niatycki Book 1980 Springer-Verlag New York Inc. 1980 Quantenmechanik.Quantisierung

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31#
發(fā)表于 2025-3-26 21:38:31 | 只看該作者
32#
發(fā)表于 2025-3-27 05:01:18 | 只看該作者
33#
發(fā)表于 2025-3-27 06:18:46 | 只看該作者
34#
發(fā)表于 2025-3-27 11:44:01 | 只看該作者
Rilka Dragneva,Kataryna WolczukThe phase space description of classical mechanics due to Hamilton is the starting point of the geometric quantization scheme. A brief review of Hamiltonian dynamics, formulated in the language of differential geometry, is given here in order to establish the notation.
35#
發(fā)表于 2025-3-27 14:04:19 | 只看該作者
36#
發(fā)表于 2025-3-27 19:33:44 | 只看該作者
EU Influence Beyond ConditionalityThe phase space χ of a single particle is isomorphic to R.. An isomorphism χ→R. is defined by the components q., q., q. of the position vector . and the components p., p., p. the linear momentum . with respect to some inertial frame. The Lagrange bracket is given by
37#
發(fā)表于 2025-3-27 23:38:05 | 只看該作者
38#
發(fā)表于 2025-3-28 02:28:38 | 只看該作者
39#
發(fā)表于 2025-3-28 08:34:41 | 只看該作者
Quantization,We describe here the process of quantizing functions f on (X, ω) which generate one-parameter groups ?.. of canonical transformations such that the pair (.?. .(F), F) of polarizations is strongly admissible.
40#
發(fā)表于 2025-3-28 10:31:33 | 只看該作者
,Schr?dinger Representation,The phase space χ of a single particle is isomorphic to R.. An isomorphism χ→R. is defined by the components q., q., q. of the position vector . and the components p., p., p. the linear momentum . with respect to some inertial frame. The Lagrange bracket is given by
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