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arXiv math-ph/0010013math-phmath.MP
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具有磁场和无界随机势的薛定谔算子积分态密度的存在唯一性

Existence and uniqueness of the integrated density of states for Schrödinger operators with magnetic fields and unbounded random potentials

Thomas Hupfer, Hajo Leschke, Peter Müller, Simone Warzel

摘要:

本文研究的对象是多维欧氏空间中量子粒子的积分态密度,该空间由具有恒定磁场和随机势的薛定谔算符表征,该势可以从上到下是无界的.对于满足简单矩条件的遍历随机势,给出了有限体积算子在不同边界条件下的空间本征值集中的无限体积极限几乎必然存在的详细证明.由于所有这些限制都与无限体积算子的空间局域谱族的迹的期望相一致,因此积分态密度几乎肯定是非随机的,并且与所选择的边界条件无关。我们证明了边界条件的独立性,并推广了S。Doi,A. Iwatsuka和T.我的[数学Z. { \bf 237}(2001)335-371]和S. Nakamura [J. Funct. Anal. { \bf 173}(2001)136-152]。

英文摘要:

The object of the present study is the integrated density of states of a quantum particle in multi-dimensional Euclidean space which is characterized by a Schrödinger operator with a constant magnetic field and a random potential which may be unbounded from above and from below. For an ergodic random potential satisfying a simple moment condition, we give a detailed proof that the infinite-volume limits of spatial eigenvalue concentrations of finite-volume operators with different boundary conditions exist almost surely. Since all these limits are shown to coincide with the expectation of the trace of the spatially localized spectral family of the infinite-volume operator, the integrated density of states is almost surely non-random and independent of the chosen boundary condition. Our proof of the independence of the boundary condition builds on and generalizes certain results by S. Doi, A. Iwatsuka and T. Mine [Math. Z. {\bf 237} (2001) 335-371] and S. Nakamura [J. Funct. Anal. {\bf 173} (2001) 136-152].

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。

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