正则变函数,广义内容,分形弦谱

T. Eichinger, S. Winter
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引用次数: 0

摘要

我们重新讨论了分形边界有界开集$\Omega\subset\mathbb{R}$上Dirichlet-Laplacian特征值分布的刻画问题。从Lapidus和Pomerance \cite{LapPo1}的结果可知,特征值计数函数的渐近第二项可以用$\Omega$边界的Minkowski含量来描述,只要它存在。他和Lapidus \cite{HeLap2}讨论了这一特征的显著扩展,即设置$\Omega$的边界不一定是闵可夫斯基可测量的。他们采用所谓的广义闵可夫斯基内容,用规范函数给出,比通常的幂函数更一般。在它们的理论中,有效规范函数的一类具有一定的技术条件,其几何意义和必要性并不明显。因此,不完全清楚该方法有多通用,以及涵盖了哪些集$\Omega$。在这里,我们重新审视这些结果,并将它们放在有规律变化的函数的上下文中。利用卡拉马塔理论,有可能摆脱大多数技术条件,简化他和拉皮德斯给出的证明,从而揭示出他们的结果的更多美丽。进一步的简化来自\cite{RW13}中闵可夫斯基含量的表征结果。我们希望我们对这些光谱问题的新观点能对这一美丽的理论进行一些进一步的研究。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Regularly varying functions, generalized contents, and the spectrum of fractal strings
We revisit the problem of characterizing the eigenvalue distribution of the Dirichlet-Laplacian on bounded open sets $\Omega\subset\mathbb{R}$ with fractal boundaries. It is well-known from the results of Lapidus and Pomerance \cite{LapPo1} that the asymptotic second term of the eigenvalue counting function can be described in terms of the Minkowski content of the boundary of $\Omega$ provided it exists. He and Lapidus \cite{HeLap2} discussed a remarkable extension of this characterization to sets $\Omega$ with boundaries that are not necessarily Minkowski measurable. They employed so-called generalized Minkowski contents given in terms of gauge functions more general than the usual power functions. The class of valid gauge functions in their theory is characterized by some technical conditions, the geometric meaning and necessity of which is not obvious. Therefore, it is not completely clear how general the approach is and which sets $\Omega$ are covered. Here we revisit these results and put them in the context of regularly varying functions. Using Karamata theory, it is possible to get rid of most of the technical conditions and simplify the proofs given by He and Lapidus, revealing thus even more of the beauty of their results. Further simplifications arise from characterization results for Minkowski contents obtained in \cite{RW13}. We hope our new point of view on these spectral problems will initiate some further investigations of this beautiful theory.
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