二维各向同性谐振子的升降算符解法

本文利用角动量算符的Ｓｃｈｗｉｎｇｅｒ表示，用代数方法研究了二维各向同性谐振子的能量本征函数．求出了（Ｈ，ｌｚ）共同本征函数　Ｎｍ（θ，）　，找到了量子数Ｎ，ｍ的升降算符以及各本征函数之间的递推关系，包括径向波函数的递推关系．给出了（Ｈ１，Ｈ２）表象与（Ｈ，ｌｚ）表象之间的变换关系，这关系和转动矩阵有密切联系．     

论双曲型方程初一边值问题和初值问题解法的统一性

作者探索把双曲型方程初一边值问题中的初始函数在相应的本征函数族下展开成为Fourier级数，把初始函数延拓到整个空间，把初一边值问题转化成为初值问题，从而使这两类不同的定解问题的解法统一起来。     

Reproducing Spaces and Localization Operators

This paper, by using of windowed Fourier transform (WFT), gives a family of embedding operators Tn:L^2(R)→L^2(C,e^-|z|^2/2dzd-↑z/4πi), s.t. TnL^2(R) lontain in L^2(C,e^-|z|^2/2dzd-↑z/4πi) are reproducing subspaces (n=0, Bargmann Space); and gives a reproducing kernel and an orthonormal basis (ONB) of TnL^2(R), Furthermore, it shows the orthogonal spaces decomposition of L^2(C,e^-|z|^2/2dzd-↑z/4πi). Finally, by using the preceding results, it shows the eigenvalues and eigenfunctions of a class of localization operators associated with WFT, which extends the result of Daubechies in [1] and [6].     

分离变量法与哈密尔顿体系

数学物理与力学中用分离变量法求解偏微分方程经常导致自共轭算子的sturmLiouville问题,在此基础上而得以展开求解。然而在应用中有大量问题并不能导致自共轭算子。本文通过最小势能变分原理,选用状态变量及其对偶变量,导向一般变分原理。利用结构力学与最优控制的模拟理论,导向哈密尔顿体系。将有限维的理论推广到相应的哈密尔顿算子矩阵及共轭辛矩阵代数的理论。拓广了经典的分离变量法,证明了全状态本征函数向量的共轭辛正交归一性质及按本征函数向量展开的理论。以条形板为例,说明了应用。     

坐标表象与任意力学量表象的关系

通过讨论坐标表象和任意力学量表象的关系,首先分析了具有连续本征值的算符本征函数δ函数归一化的由来,在此基础上研究得出一个结论,即任意力学量算符在坐标表象中的本征函数和坐标算符在任意力学量表象中的本征函数互为共轭复数,又根据这个结论对本征函数封闭性的物理意义做了一种新的解释.     

撕裂模方程的数值分析

从数值计算的角度，讨论了撕裂模方程的解。用龙格－库塔方法计算了撕裂模（2／1模）的本征函数及其连接参数。计算结果同Wesson的结果符合得很好。     

A COMPREHENSIVE PROOF OF THE GREENBERGER-HORNE-ZEILINGER THEOREM FOR THE FOUR-QUBIT SYSTEM

Greenberger-Horne-Zeilinger(GHZ)theorem asserts that there is a set of mutually commuting nonlocal observables with a common eigenstate on which those ob- servables assume values that refute the attempt to assign values only required to have them by the local realism of Einstein,Podolsky,and Rosen(EPR).It is known that for a three-qubit system.there is only one form of the GHZ-Mermin-like argument with equiva- lence up to a local unitary transformation,which is exactly Mermin's version of the GHZ theorem.This article for a four-qubit system,which was originally studied by GHZ,the authors show that there are nine distinct forms of the GHZ-Mermin-like argument.The proof is obtained using certain geometric invariants to characterize the sets of mutually commuting nonlocal spin observables on the four-qubit system.It is proved that there are at most nine elements(except for a different sign)in a set of mutually commuting nonlocal spin observables in the four-qubit system,and each GHZ-Mermin-like argument involves a set of at least five mutually commuting four-qubit nonlocal spin observables with a GHZ state as a common eigenstate in GHZ's theorem.Therefore,we present a complete construction of the GHZ theorem for the four-qubit system.     

一种新的阶跃折射率光纤本征函数表达形式

为了阐明阶跃折射率光纤的模式特性,根据电磁波辐射的能量守恒定律和经过狄拉克函数奇异性修正的亥姆霍兹方程,通过数学推导和证明得出:柱面径向行波场的本征函数是经过狄拉克函数修正的整数阶汉克尔函数,阶跃折射率光纤模式场的本征函数是零、一阶贝塞尔函数经过狄拉克函数修正的零、一阶诺埃曼函数和虚参量汉克尔函数.该结论揭示了光纤芯层和包层模式场分别是径向驻波场和倏逝波场的本质,并基此推导出新的光纤模式特征方程,模式存在条件,模式数目和符合光纤实际的基模归一化截止频率的理论值.