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Transverse intersection of invariant manifolds in perturbed multi-symplectic systems

机译:扰动多辛系统中不变流形的横向相交

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A multi-symplectic system is a PDE with a Hamiltonian structure in both temporal and spatial variables. This article considers spatially periodic perturbations of symmetric multi-symplectic systems. Due to their structure, unperturbed multi-symplectic systems often have families of solitary waves or front solutions, which together with the additional symmetries lead to large invariant manifolds. Periodic perturbations break the translational symmetry in space and might break some of the other symmetries as well. In this article, periodic perturbations of a translation invariant PDE with a one-dimensional symmetry group are considered. It is assumed that the unperturbed PDE has a three-dimensional invariant manifold associated with a solitary wave or front connection of multi-symplectic relative equilibria. Using the momentum associated with the symmetry group, sufficient conditions for the persistence of invariant manifolds and their transversal intersection are derived. In the equivariant case, invariance of the momentum under the perturbation gives the persistence of the full three-dimensional manifold. In this case, there is also a weaker condition for the persistence of a two-dimensional submanifold with a selected value of the momentum. In the non-equivariant case, the condition leads to the persistence of a one-dimensional submanifold with a seleceted value of the momentum and a selected action of the symmetry group. These results are applicable to general Hamiltonian systems with double zero eigenvalue in the linearization due to continuous symmetry. The conditions are illustrated on the example of the defocussing non-linear Schrodinger equations with perturbations which illustrate the three cases. The perturbations are: an equivariant Hamiltonian perturbation which keeps the momentum level sets invariant; an equivariant damped, driven perturbation; and a perturbation which breaks the rotational symmetry.
机译:多符号系统是在时间和空间变量上均具有哈密顿结构的PDE。本文考虑了对称多辛系统的空间周期扰动。由于其结构,不受干扰的多辛系统通常具有孤立波或前解的族,这与附加的对称性一起导致了大型不变流形。周期性扰动破坏了空间的平移对称性,也可能破坏了其他一些对称性。在本文中,考虑具有一维对称群的平移不变PDE的周期性扰动。假定不受扰动的PDE具有三维不变歧管,该多维不变歧管与孤立的波或多辛的相对平衡的前连接有关。利用与对称群相关的动量,推导了不变流形及其横向相交的持续性的充分条件。在等变情况下,扰动下动量的不变性给出了完整三维流形的持久性。在这种情况下,具有选定动量值的二维子流形的持久性也较弱。在非等变情况下,该条件会导致一维子流形的持续存在,其动量的选择值高且对称组具有选定的作用。这些结果适用于由于连续对称而在线性化中具有双零特征值的一般哈密顿系统。在带有扰动的散焦非线性Schrodinger方程的示例中说明了这些条件,这些示例说明了三种情况。这些扰动是:使动量水平集保持不变的等变哈密顿扰动;等变的阻尼驱动扰动;扰动破坏了旋转对称性。

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