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Stability and motion laws for Ginzburg-Landau vortices on manifolds under dissipative and conservative dynamics.

机译:耗散和保守动力学下流形上的Ginzburg-Landau涡旋的稳定性和运动定律。

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摘要

We consider the Ginzburg-Landau energy on compact, simply-connected 2-manifolds. Here we mainly address three problems that involve vortices. One is the stability or instability of critical points of the Ginzburg-Landau energy in the sense of positivity or not of the second variation. A second is the vortex dynamics for the Ginzburg-Landau heat flow, both in the asymptotic regime where the parameter epsilon attends to zero and for fixed epsilon. The third is a similar analysis of vortex motion for the Gross-Pitaevskii equation.;Our first main result is that for compact, simply connected 2-manifolds without boundary, any non-constant critical points must be unstable when epsilon is small if at least one limiting vortex is located at a point of positive Gauss curvature. Furthermore, on a surface of revolution with non-zero Gauss curvature at at least one of the poles, we argue that all critical points are unstable for small epsilon, regardless of the curvature at the limiting vortex locations.;For the Ginzburg-Landau heat flow, we show the vortices of a solution evolve according to the gradient flow of the renormalized energy. We then specialize to the case on a sphere and study the limiting system of ODE's and establish an annihilation result. After that we return to the Ginzburg-Landau heat flow on a sphere and derive some weighted energy identities. Finally we prove the annihilation result for the PDE setting on a surface of revolution with boundary.;For the Gross-Pitaevskii equation, we show the vortices of a solution follow the Hamiltonian point-vortex flow associated with the renormalized energy. Then on surfaces of revolution, we find rotating periodic solutions to the generalized point-vortex problem and seek a rotating solution to the Gross-Pitaevskii equation having vortices that follow those of the point-vortex flow for epsilon sufficiently small.
机译:我们考虑在紧凑的,简单连接的2流形上的Ginzburg-Landau能量。在这里,我们主要解决涉及涡旋的三个问题。第一个是从第二个变化的积极性或不积极性的角度来看,Ginzburg-Landau能量的临界点的稳定性或不稳定性。第二个是金兹堡-兰道热流的涡旋动力学,在渐进状态下参数ε趋于零,在固定ε上。第三是对Gross-Pitaevskii方程的涡旋运动进行的类似分析;我们的第一个主要结果是,对于紧凑,简单连接的无边界的2流形,当epsilon小时,如果至少至少有非恒定临界点必须是不稳定的一个极限旋涡位于高斯正曲率点。此外,在至少一个极点上具有非零高斯曲率的旋转表面上,我们认为对于小ε来说,所有临界点都是不稳定的,而不管极限涡旋位置处的曲率如何。流,我们显示了解决方案的涡旋根据重新归一化能量的梯度流而演化。然后,我们专门研究球面上的情况,研究ODE的极限系统并确定establish灭结果。之后,我们返回球上的金茨堡-朗道热流,并得出一些加权的能量恒等式。最后,我们证明了带边界旋转表面上的PDE设定的hil灭结果。对于Gross-Pitaevskii方程,我们显示了伴随重整化能量的哈密顿点涡流遵循解的涡旋。然后,在旋转的表面上,我们找到了广义点涡旋问题的旋转周期解,并找到了具有涡旋的Gross-Pitaevskii方程的旋转解,该涡旋的涡旋遵循点旋涡流的足够小。

著录项

  • 作者

    Chen, Ko-Shin.;

  • 作者单位

    Indiana University.;

  • 授予单位 Indiana University.;
  • 学科 Mathematics.
  • 学位 Ph.D.
  • 年度 2014
  • 页码 87 p.
  • 总页数 87
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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