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Lectures on wave invariants

机译:波浪不变的讲座

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These are notes of some lectures on ave invariants and quantum normal form invariants of the Laplacian Δ at a closed geodesic γ of a compact boundaryless Riemannian manifold (M,g). Our purpose in the lectures was to give a survey of some recent developments involving these invariants and their applications to inverse spectral theory, mainly following the references [G.1] [G.2] [Z.1][Z.2][Z.3]. Originally, the notes were intended to mirror the lectures but in the intervening time we wrote another expository account on this topic [Z.4] and also extended the methods and applications to certain plane domains which were outside the scope of the original lectures [Z.5]. These events seemed to render the original notes obsolete. In their place, we have included some related but more elementary material on wave invariants and normal forms which do not seem to have been published before and which seem to us to have some pedagogical value. This material consists first of the calculation of wave invariants on manifolds without conjugate points using a global Hadamard-Riesz parametrix. Readers who are more familiar with heat kernels than wave kernels may find this calculation an easy-to-read entree into wave invariants. A short section on normal forms leads the reader into this more sophisticated - and more useful - approach to wave invariants. We illustrate this approach by putting a Sturm-Liouville operator on a finite interval (with Dirichlet boundary conditions) into normal form. The results are equivalent to the classical expansions of the eigenvalues and eigenfunctions as described in Marchenko [M] and Levitan-Sargsjan [LS], but the approach is quite different and possibly new. The main point is that it generalizes to higher dimensions. We hope the reader will find it stimulating to compare the (well-understood) one-dimensional case to the (still murky) higher dimensional ones. To highlight the murkiness we end these notes with a few open problems.
机译:这些是在紧凑型无边缘riemannian歧管(M,G)的闭合测地γ处的Laplacianδ的某些讲义的注意事项。我们在讲座中的目的是对一些涉及这些不变性的发展以及他们的应用到逆频谱理论的一些可能进行调查,主要遵循参考文献[g.1] [z.1] [z.2] [ Z.3]。最初,笔记旨在镜像讲座,但在中间时间我们在本主题[z.4]上写了另一个展示账户,并将方法和应用扩展到了在原始讲座范围之外的某些平面域[z .5]。这些事件似乎使原始注释过时。在他们的位置,我们已经包括一些相关但更多的初级材料在波不变量和正常形式上,这似乎没有发布,似乎我们有一些教学价值。该材料首先在没有使用全球Hadamard-Riesz parametrix的情况下计算歧管上的波浪不变的计算。更熟悉热核的读者比Wave内核可能会发现此计算易于阅读的主体进入Wave Invariants。正常形式的简短段导致读者进入更复杂 - 更有用的 - 波浪不变的方法。我们通过将Sturm-Liouville运算符放在有限间隔(具有Dirichlet边界条件)中以正常形式来说明这种方法。结果相当于Marchenko [M]和Levitan-Sargsjan [LS]中所述的特征值和特征障碍的经典扩展,但方法是完全不同的,并且可能是新的。主要观点是它推广到更高的维度。我们希望读者能够发现它刺激(井理解)一维案件到(仍然是Myky)更高的维度。要突出杂音,我们将通过一些公开问题结束这些笔记。

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