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arXiv 2006.15230math-phmath.MP
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图上确定性薛定谔算子势的态密度外测度依赖性及其在遍历和随机模型中的应用

Dependence of the density of states outer measure on the potential for deterministic Schrödinger operators on graphs with applications to ergodic and random models

Peter D. Hislop, Christoph A. Marx

摘要:

我们继续研究薛定谔算符的态密度测度和相关谱函数对势的依赖性。而我们早期的工作集中在随机薛定谔算子,我们将这些结果扩展到薛定谔算子的无限图的确定性潜力和遍历潜力,并改进我们的结果为随机潜力。特别地,我们证明了格点上随机薛定谔算子的DOSm的Lipschitz连续性,恢复了\cite{kachkovskiy, shamis}的结果.对于我们的治疗确定性的潜力,我们首先研究的状态密度外测量(DOSoM),定义为所有薛定谔算子,并证明了一个确定性的结果的连续模的DOSoM相对于潜在的。我们将这些结果应用于格$Z^d$和Bethe格上的薛定谔算子。在前一种情况下,我们证明了DOSoM的Lipschitz连续性,在后一种情况下,我们证明了DOSoM是$\frac{1}{2}$ -log-Hölder连续的。我们的技术结合了一个新的有限范围的减少,使我们能够研究的DOSoM和相关功能的依赖性,只有有限多的变量和捕获的几何图形在无穷远的单参数家庭的自伴算子的抽象Lipschitz属性。

英文摘要:

We continue our study of the dependence of the density of states measure and related spectral functions of Schrödinger operators on the potential. Whereas our earlier work focused on random Schrödinger operators, we extend these results to Schrödinger operators on infinite graphs with deterministic potentials and ergodic potentials, and improve our results for random potentials. In particular, we prove the Lipschitz continuity of the DOSm for random Schrödinger operators on the lattice, recovering results of \cite{kachkovskiy, shamis}. For our treatment of deterministic potentials, we first study the density of states outer measure (DOSoM), defined for all Schrödinger operators, and prove a deterministic result of the modulus of continuity of the DOSoM with respect to the potential. We apply these results to Schrödinger operators on the lattice $Z^d$ and the Bethe lattice. In the former case, we prove the Lipschitz continuity of the DOSoM, and in the latter case, we prove that the DOSoM is $\frac{1}{2}$-log-Hölder continuous. Our technique combines the abstract Lipschitz property of one-parameter families of self-adjoint operators with a new finite-range reduction that allows us to study the dependency of the DOSoM and related functions on only finitely-many variables and captures the geometry of the graph at infinity.

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