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Conformal maps, monodromy transformations, and non-reversible Hamiltonian systems - MaRDI portal

Conformal maps, monodromy transformations, and non-reversible Hamiltonian systems (Q1588363)

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scientific article; zbMATH DE number 1539313
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Conformal maps, monodromy transformations, and non-reversible Hamiltonian systems
scientific article; zbMATH DE number 1539313

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    Conformal maps, monodromy transformations, and non-reversible Hamiltonian systems (English)
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    12 December 2001
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    The following main result is presented: Theorem. For \(n\geq 2\), there exist non-weakly reversible Hamiltonian vector fields \[ \sum-H_{y_j} {\partial \over \partial x_j}+ H_{x_j}{\partial \over\partial y_j} \] of the form \(H(x,y)= \sum^n_{j=1} \alpha_j(x_j^2 +y^2_j) +0(3)\), for which \(\alpha_1 \alpha_2<0\), and \(\alpha_1, \dots, \alpha_n\) are non-resonant.
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    Hamiltonian systems
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    conformal maps
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    non-reversible vector fields
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