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arXiv 1302.4142math-phmath.MP
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稳态散射理论的构造性方法

A constructive approach to stationary scattering theory

Nurulla Azamov

摘要:

本文给出了Hilbert空间$\mathcal H$上满足下列条件的自伴算子对$H_0$和$H_1$的平稳散射理论的一种新的构造性方法:(i)对于$\mathbb R,$的任何开有界子集$Δ$,算子$F E_Δ^{H_0}$和$F E_Δ^{H_1}$是Hilbert-Schmidt,并且(ii)$V = H_1- H_0$是有界的,并允许分解$V = F^*JF,$,其中$F$是从$\mathcal H$到另一个Hilbert空间$\mathcal K$的具有平凡核的有界算子,$J$是有界自$\mathcal K.$上的伴随算子满足这些条件的一对算子的例子是作用在$L^2(\mathbb R^ν),$上的薛定谔算子$H_0 = -Δ+ V_0$,其中$V_0$是类$K_ν$的势(参见B. Simon,{ \it Schrödinger semigrops,} Bull. AMS 7,1982,447- 526)和$H_1 = H_0 + V_1,$,其中$V_1 \in L^\infty(\mathbb R^ν) \cap L^1(\mathbb R^ν).$本文的结果是波算子$W_\pm(H_1,H_0)$的存在性和完备性的一个新的证明以及散射矩阵的定态公式的一个新的构造性证明。这种散射理论的方法是基于显式对角化的自伴算子$H$的希尔伯特空间层$\EuScript S(H,F)$与对$(H,F)$和随后的建设和研究之间的纤维$\mathfrak h_λ(H_0,F)$和$\mathfrak h_λ(H_1,F)$层$\EuScript S(H_0,F)$和$\EuScript S(H_1,F)$分别作用的波矩阵$w_\pm(λ; H_1,H_0)$的性质。波算子$W_\pm(H_1,H_0)$被定义为波矩阵的直接积分,并证明了它与经典的含时波算子定义是一致的。

英文摘要:

In this paper we give a new and constructive approach to stationary scattering theory for pairs of self-adjoint operators $H_0$ and $H_1$ on a Hilbert space $\mathcal H$ which satisfy the following conditions: (i) for any open bounded subset $Δ$ of $\mathbb R,$ the operators $F E_Δ^{H_0}$ and $F E_Δ^{H_1}$ are Hilbert-Schmidt and (ii) $V = H_1- H_0$ is bounded and admits decomposition $V = F^*JF,$ where $F$ is a bounded operator with trivial kernel from $\mathcal H$ to another Hilbert space $\mathcal K$ and $J$ is a bounded self-adjoint operator on $\mathcal K.$ An example of a pair of operators which satisfy these conditions is the Schrödinger operator $H_0 = -Δ+ V_0$ acting on $L^2(\mathbb R^ν),$ where $V_0$ is a potential of class $K_ν$ (see B.\,Simon, {\it Schrödinger semigroups,} Bull. AMS 7, 1982, 447--526) and $H_1 = H_0 + V_1,$ where $V_1 \in L^\infty(\mathbb R^ν) \cap L^1(\mathbb R^ν).$ Among results of this paper is a new proof of existence and completeness of wave operators $W_\pm(H_1,H_0)$ and a new constructive proof of stationary formula for the scattering matrix. This approach to scattering theory is based on explicit diagonalization of a self-adjoint operator $H$ on a sheaf of Hilbert spaces $\EuScript S(H,F)$ associated with the pair $(H,F)$ and with subsequent construction and study of properties of wave matrices $w_\pm(λ; H_1,H_0)$ acting between fibers $\mathfrak h_λ(H_0,F)$ and $\mathfrak h_λ(H_1,F)$ of sheaves $\EuScript S(H_0,F)$ and $\EuScript S(H_1,F)$ respectively. The wave operators $W_\pm(H_1,H_0)$ are then defined as direct integrals of wave matrices and are proved to coincide with classical time-dependent definition of wave operators.

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