一类自伴随算子的奇异有限秩非对称微扰

O. Dyuzhenkova, M. Dudkin
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引用次数: 0

摘要

dudkin M.E.和Vdovenko T.I. \cite{k8,k9}首次考虑了${\mathcal H}_{-1}$和${\mathcal H}_{-2}$类自伴随算子的奇异非对称秩1摄动。在上述论文中,描述了在这种扰动中发生的点谱的一些性质。本文推广了在有限秩的非对称类${\mathcal H}_{-2}$扰动情况下\cite{k8,k9}和\cite{k2}的结果。也就是说,下面的形式表达式被认为是\begin{equation*}\tilde A=A+\sum \limits_{j=1}^{n}\alpha_j\langle\cdot,\omega_j\rangle\delta_j,\end{equation*},其中$A$是可分离希尔伯特空间上的一个非摄动自共轭算子,${\mathcal H}$, $\alpha_j\in{\mathbb C}$, $\omega_j$, $\delta_j$, $j=1,2, ..., n<\infty$是由算子$A$构造的负空间中的向量,${\mathcal H}_{-2}$, $\langle\cdot,\cdot\rangle$是正负空间之间的对偶标量积。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
SINGULARLY FINITE RANK NONSYMMETRIC PERTURBATIONS ${\mathcal H}_{-2}$-CLASS OF A SELF-ADJOINT OPERATOR
The singular nonsymmetric rank one perturbation of a self-adjoint operator from classes ${\mathcal H}_{-1}$ and ${\mathcal H}_{-2}$ was considered for the first time in works by Dudkin M.E. and Vdovenko T.I. \cite{k8,k9}. In the mentioned papers, some properties of the point spectrum are described, which occur during such perturbations. This paper proposes generalizations of the results presented in \cite{k8,k9} and \cite{k2} in the case of nonsymmetric class ${\mathcal H}_{-2}$ perturbations of finite rank. That is, the formal expression of the following is considered \begin{equation*} \tilde A=A+\sum \limits_{j=1}^{n}\alpha_j\langle\cdot,\omega_j\rangle\delta_j, \end{equation*} where $A$ is an unperturbed self-adjoint operator on a separable Hilbert space ${\mathcal H}$, $\alpha_j\in{\mathbb C}$, $\omega_j$, $\delta_j$, $j=1,2, ..., n<\infty$ are vectors from the negative space ${\mathcal H}_{-2}$ constructed by the operator $A$, $\langle\cdot,\cdot\rangle$ is the dual scalar product between positive and negative spaces.
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