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A non-symplectic generalization of Hamiltonian mechanics is considered. It allows include into consideration “non-Lagrange” systems, such as theory of charged particle in the field of magnetic monopole. The corresponding generalization for the Fedosov manifolds is given. The structure of phase space of “charged particle in the field of magnetic monopole” is studied.

生成讲解博客的中文版本

生成AI智能校验的中文版本