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The main result of this paper is the discretization of Hamiltonian systems of the form , where is a constant symmetric matrix and is a polynomial of degree in any number of variables . The discretization uses the method of polarization and preserves both the energy and the invariant measure of the differential equation, as well as the dimension of the phase space. This generalises earlier work for discretizations of first order systems with , and of second order systems with and .

生成讲解博客的中文版本

生成AI智能校验的中文版本