
The author considers the discrete Hamiltonian system \[ \Delta x(t)= H_u(t,x(t+1),u(t)), \qquad \Delta u(t)= -H_x(t,x(t+1),u(t)), \tag{1} \] where \(x,u\in \mathbb R^d\), \(H(t,x,u)\) is the corresponding real Hamiltonian function having continuous derivatives in \(x\), \(u\). The author shows that the discrete nonlinear Hamiltonian system (1) is of symplectic structure. As a result its phase flow is a discrete one-parameter family of symplectic transformations preserving the phase volume. Especially, in the autonomous case, its phase flow is a discrete one-parameter group of symplectic transformations. The results are related to an open problem in \textit{C. D. Ahlbrandt} [ibid. 180, No.~2, 498--517 (1993; Zbl 0802.39005)].
Discretization methods and integrators (symplectic, variational, geometric, etc.) for dynamical systems, Relations of dynamical systems with symplectic geometry and topology, symplectic transformations, symplectic structure, Applied Mathematics, discrete Hamiltonian system, Discrete version of topics in analysis, phase flow, Analysis
Discretization methods and integrators (symplectic, variational, geometric, etc.) for dynamical systems, Relations of dynamical systems with symplectic geometry and topology, symplectic transformations, symplectic structure, Applied Mathematics, discrete Hamiltonian system, Discrete version of topics in analysis, phase flow, Analysis
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