关于J－对称微分算子的J－自伴扩张的若干注记

本文给出了一条解析描述Ｊ－对称微分算子Ｊ－自伴扩张的新途径．我们借助方程Ｔ（ｙ）＝λｏｙ的解，而不是如文［３］利用方程＋（ｙ）＇＝－ｙ的解来描述Ｊ－对称微分算式的所有Ｊ－自伴域在奇异端点的边条件，不过我们假设生成的最小算子具非空正则域．我们对主要定理给出了若干有趣的注，得到了二阶极限圆情形的有趣结果．     

奇异向量微分算子的自伴域

本文在向量值函数空间中,推广应用最大算子域的直和分解法,讨论奇异向量微分算子的自伴扩张问题,给出了奇异形式对称向量微分算式一切自伴扩张域的完全描述,概括了[1—4]的相应结果.     

复系数2n阶微分算子的谱

本文研究了复系数２ｎ阶微分算式（２．１）生成的Ｊ－自伴微分算子谱,对两类微分算子的本质谱,离散谱作了定性研究,得到了所生成微分算子本质谱的存在范围,以及所生成微分算子的谱是离散的充分条件．     

高阶常型微分算子自伴域的辛几何刻划

考虑高阶常型实系数微分算子ι(y)=n↑∑↑k=0(pn-ky^(κ))^(κ)(x∈[α,b])。利用辛几何，对ι（y）的自伴域进行了分类，给出了ι（y）自伴域是κ－级的充要条件（0≤κ≤n）。     

亏指数为可数无穷的对称微分算子的自伴扩张

应用Ｈｉｌｂｅｒｔ空间内对称算子自伴域一种新的描述方法，得到直和空间内亏指数为可数无穷的对称微分算子自伴扩张的完全解析描述。     

奇型微分算子极大增生性的解析刻画

考虑奇型实系数微分算式ｌ（ｙ）＝（－１）~ｊ（ｐｎ（ｘ）ｙ（ｊ）（ｘ）在函数空间Ｌ２［ａ］上,本文借助边界条件刻画了ｌ（ｙ）生成极大增生算子的充要条件,及其ｌ（ｙ）最小生成算子为非负自伴扩张的充要条件．     

m个微分算式乘积的自伴边界条件

本文假设n阶正则对称微分算式l(y)的幂算式l~m(y)在L~2[α,∞)中是部分分离的,首先刻画了由幂算式l~m(y)生成的微分算子T(l~m)的自伴边界条件．然后,在L~2[α,∞)中,借助T(l~m)的自伴域的这种刻画形式,研究了m个由n阶微分算式l(y)生成的微分算子T_k(l)(k=1,2,……,m；m∈z,m≥2)乘积的自伴性问题,获得了乘积算子T_m(l)…T_2(l)T_1(l)是自伴算子的充要条件．     

J—自共轭微分算子谱的定性分析

本文对J－自共轭微分算子谱理论研究情况做一些概要性的介绍,第一部分简要回顾了J－自共轭微分算子理论研究的发展过程,第二,三部分介绍了J－自共轭微分算子的本质谱和离散谱定性分析的主要方法和结论;第四部分扼要叙述J－自共轭微分算子其它方面的一些工作,以及J－自共轭微分算子谱理论研究中尚待解决的问题。     

2n阶微分算子乘积自伴的充分必要条件

给定Hilbert空间L2[a,∞)上两个由2n阶对称微分算式生成的微分算子Li(i=1,2),该文给出了乘积算子L2L1是自伴算子的一个充分必要条件．     

一类极限点型的J-对称微分算子

本文利用纳依玛克 ~［１］的方法研究了 ２ｎ阶非对称微分算子（Ｊ－对称微分算 子）;得到一类极限点型的非对称微分算子（Ｊ－对称微分算子）．     

向量值函数空间中J-对称算子的J-自伴延拓

给出了向量值函数空间中J-对称算子的J-自伴延拓的完全解析描述.我们应用Knowles理论,借助方程τ(y)=λ     

一类具有转移条件高阶微分算子的J-自伴性

本文研究了一类具有转移条件的高阶复系数微分算子的J-自伴性,利用J-对称微分算式的拉格朗日双线性型、J-自伴算子的定义及矩阵表示的方法,证明了这类微分算子是J-自伴的,且对应于不同特征值的特征向量和特征子空间都是C-正交的.     

J-selfadjointness of a class of high-order differential operators with transmission conditions

This paper is to investigate the J-selfadjointness of a class of high-order complex coefficients differential operators with transmission conditions. Using the Lagrange bilinear form of J-symmetric differential equations, the definition of J-selfadjoint differential operators and the method of matrix representation, we prove that the operator is J-selfadjoint operator, and the eigenvectors and eigen-subspaces corresponding to different eigenvalues are C-orthogonal.     

A REPRESENTATION FORMULA RELATED TO SCHR(O)DINGER OPERATORS

Schr(o)dinger operator is a central subject in the mathematical study of quantum mechanics.Consider the Schrodinger operator H = -△ V on R, where △ = d2/dx2 and the potential function V is real valued. In Fourier analysis, it is well-known that a square integrable function admits an expansion with exponentials as eigenfunctions of -△. A natural conjecture is that an L2 function admits a similar expansion in terms of "eigenfunctions" of H, a perturbation of the Laplacian (see [7], Ch. Ⅺ and the notes), under certain condition on V.     

On a class of self-similar processes with stationary increments in higher order Wiener chaoses

We study a class of self-similar processes with stationary increments belonging to higher order Wiener chaoses which are similar to Hermite processes. We obtain an almost sure wavelet-like expansion of these processes. This allows us to compute the pointwise and local Hölder regularity of sample paths and to analyse their behaviour at infinity. We also provide some results on the Hausdorff dimension of the range and graphs of multidimensional anisotropic self-similar processes with stationary increments defined by multiple Wiener–Itô integrals.     

On a class of Riemann surfaces

It is considered the class of Riemann surfaces with dimT1 = 0, where T1 is a subclass of exact harmonic forms which is one of the factors in the orthogonal decomposition of the spaceΩH of harmonic forms of the surface, namely The surfaces in the class OHD and the class of planar surfaces satisfy dimT1 = 0. A.Pfluger posed the question whether there might exist other surfaces outside those two classes. Here it is shown that in the case of finite genus g, we should look for a surface S with dimT1 = 0 among the surfaces of the form Sg\K , where Sg is a closed surface of genus g and K a compact set of positive harmonic measure with perfect components and very irregular boundary.