Let $X=\mathbb{R}\times M$ be the spacetime, where $M$ is a closed manifold
equipped with a Riemannian metric $g$, and we consider a symmetric Klein-Gordon
type operator $P$ on $X$, which is asymptotically converges to
$\partial_t^2-\triangle_g$ as $|t|\to\infty$, where $\triangle_g$ is the
Laplace-Beltrami operator on $M$. We prove the essential self-adjointness of
$P$ on $C_0^\infty(X)$. The idea of the proof is closely related to a recent
paper by the authors on the essential self-adjointness for Klein-Gordon
operators on asymptotically flat spaces.
Here we discuss a new simplified proof of the essential self-adjointness for
formally self-adjoint differential operators of real principal type, previously
proved by Vasy (2020) and Nakamura-Taira (2021). For simplicity, here we
discuss the second order cases, i.e., Klein-Gordon type operators only.
We consider the quantum graph Hamiltonian on the square lattice in Euclidean
space, and we show that the spectrum of the Hamiltonian converges to the
corresponding Schrödinger operator on the Euclidean space in the continuum
limit, and that the corresponding eigenfunctions and eigenprojections also
converge in some sense. We employ the discrete Schrödinger operator as the
intermediate operator, and we use a recent result by the second and third
author on the continuum limit of the discrete Schrödinger operator.
We propose a method of data quantization of finite discrete-time signals
which optimizes the error estimate of low frequency Haar coefficients. We also
discuss the error/noise bounds of this quantization in the Fourier space. Our
result shows one can quantize any discrete-time analog signal with high
precision at low frequencies. Our method is deterministic, and it employs no
statistical arguments, nor any probabilistic assumptions.
We consider scattering matrix for Schr\"odinger-type operators on $R^d$ with<br />
perturbation $V(x)=O(\langle x\rangle^{-1})$ as $|x|\to\infty$. We show that<br />
the scattering matrix (with time-independent modifiers) is a pseudodifferential<br />
operator. We present examples of which the spectrum of the scattering matrix is<br />
dense point spectrum.