arXivDaily arXiv每日学术速递 周一至周五更新
arXiv周末暂无论文更新,休息一下吧,周末愉快~~
arXiv 2201.00683math.DSmath-phmath.MP
收藏

弹子球系统的动力zeta函数

Dynamical zeta functions for billiards

Yann Chaubet, Vesselin Petkov

AI总结:

该研究针对外区域弹子球系统的动力zeta函数,证明其在非蚀条件下可亚纯延拓至全复平面,还得到实解析边界下Dirichlet型zeta函数非整、对应共振带含无穷多共振及下界的结论。

摘要:

设$D \subset {\mathbb R}^d,\\: d \geqslant 2$是有限个两两不交的严格凸紧障碍物的并集。设$μ_j \in {\mathbb C},\\: {\rm Im}\\: μ_j > 0$是$D$外部拉普拉斯算子在$\partial D$上满足Neumann(诺伊曼)或Dirichlet(狄利克雷)边界条件时的共振。对于奇数维$d$,$u(t) = \sum_j e^{i |t| μ_j}$是$ \mathcal{D}'({\mathbb R} \setminus \{0\})$中的分布,$u(t)$的主导奇点的拉普拉斯变换分别给出对应Neumann和Dirichlet边界条件的动力zeta函数$η_{\mathrm N}$、$η_{\mathrm D}$。这些zeta函数在共振分布分析中发挥关键作用。在非蚀条件(1.1)下,对于$d \geqslant 2$,我们证明$η_{\mathrm N}$和$η_\mathrm D$可亚纯延拓到整个复平面。在边界$\partial D$为实解析的特殊情形下,利用Fried (1995)的结果,我们证明$η_\mathrm{D}$不可能是整函数。结合Ikawa (1988)的结果,这意味着存在带状区域$\{z \in {\mathbb C}: \\: 0 < {\rm Im}\\: z \leqα\}$,其中包含Dirichlet问题的无穷多个共振$μ_j$。此外,对于$α\gg 1$,我们得到了该带状区域内共振数的一个下界。

英文摘要:

Let $D \subset {\mathbb R}^d,\: d \geqslant 2,$ be the union of a finite collection of pairwise disjoint strictly convex compact obstacles. Let $μ_j \in {\mathbb C},\: {\rm Im}\: μ_j > 0,$ be the resonances of the Laplacian in the exterior of $D$ with Neumann or Dirichlet boundary condition on $\partial D$. For $d$ odd, $u(t) = \sum_j e^{i |t| μ_j}$ is a distribution in $ \mathcal{D}'({\mathbb R} \setminus \{0\})$ and the Laplace transforms of the leading singularities of $u(t)$ yield the dynamical zeta functions $η_{\mathrm N},\: η_{\mathrm D}$ for Neumann and Dirichlet boundary conditions, respectively. These zeta functions play a crucial role in the analysis of the distribution of the resonances. Under the non-eclipse condition (1.1), for $d \geqslant 2$ we show that $η_{\mathrm N}$ and $η_\mathrm D$ admit a meromorphic continuation to the whole complex plane. In the particular case when the boundary $\partial D$ is real analytic, by using a result of Fried (1995), we prove that the function $η_\mathrm{D}$ cannot be entire. Following the result of Ikawa (1988), this implies the existence of a strip $\{z \in {\mathbb C}: \: 0 < {\rm Im}\: z \leqα\}$ containing an infinite number of resonances $μ_j$ for the Dirichlet problem. Moreover, for $α\gg 1$ we obtain a lower bound for the resonances lying in this strip.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑