在平面抛物线坐标系中求解二维氢原子的Stark效应

在平面抛物线坐标系中计算了二维氢原子的Ｓｔａｒｋ效应，得到了计算任意能级的一阶、二阶和三阶修正的普遍公式。     

二维变折射率介质辐射传递的近似模型

发展了二维梯度折射率介质热辐射传递求解的两种近似模型,线性折射率bar模型和混合bar模型.对于辐射能传递路径的求解,涉及到四个坐标系的转换:系统坐标系、网格坐标系、网格旋转坐标系和散射的当地坐标系.同时假设辐射能在每个网格内是在平面内传递.通过这两个模型的建立和新的假设条件,对于二维梯度折射率介质的热辐射传递求解的一系列问题均可较为容易地求解.     

二维耦合量子谐振子的本征值和本征函数

运用广义线性量子变换理论,给出一类二维耦合量子谐振子的能量本征值、本征函数、坐标和动量算符在能量表象中的矩阵元及演化算符.     

二维各向同性变频率谐振子的超对称性及其不变量的超对称量子力学精确解

采用超对称量子力学与不变量相结合的方法讨论了二维各向同性变频率谐振子,给出了二维各向同性变频率谐振子的不变量,采用超对称量子力学方法精确求解了不变量的本征值和本征函数,并且给出了当频率恒定时,二维常频率谐振子的本征值和本征函数的精确解.最后对不变量的超对称性进行了讨论.     

二维高斯波束对多层球粒子电磁散射的解析解

基于矢量波函数在球和柱坐标系中表达式之间的转换关系，提出了一种求解球坐标系中二维高斯波束波形因子的方法，得到了二维高斯波束波形因子在球坐标系中的解析公式.结合广义米理论推导了在轴二维高斯波束入射多层球粒子的电磁散射的解析解，并对散射强度随散射角的分布进行了数值模拟，结果与平面波入射情况进行了比较.     

基于近似Riemann解的有限体积ALE方法

研究二维平面坐标系和二维轴对称坐标系中四边形网格上可压缩流体力学的有限体积ALE(Arbitrary Lagrangian Eulerian)方法.数值方法采用节点中心有限体积法,数值通量采用适用于任意状态方程的HLLC(Harten-Lax-Van Leer-Collela)通量.空间二阶精度通过用WENO(weighted essentially non-oscillatory)方法对原始变量进行重构获得,时间离散采用两步显式Runge-Kutta格式.数值例子显示,方法具有良好的激波分辨能力和高精度的数值逼近能力.     

运动目标时空频信号变换与多维信息关联

提出了一种针对水中匀速直线运动目标的时空频信号变换方法。首先对接收信号作时频分析和频域波束形成,根据选定的目标航向对频率-方位-时间三维信号空间中的接收信号进行由基阵坐标系到目标坐标系的视在方位变换,使目标线谱信号由三维空间轨迹变换为变换域中对应平面切片上的二维轨迹,该切片由频率与方位信息联合构成的轴和时间轴构成。研究结果表明,该方法能够在变换后的信号空间中将目标线谱信号的三维轨迹转换为相应切片上的二维轨迹,相比三维信号空间更容易获得多维信息联合处理的信号处理增益。     

二维高斯波束对多层球粒子电磁散射的解析解

基于矢量波函数在球和柱坐标系中表达式之间的转换关系,提出了一种求解球坐标系中二维高斯波束波形因子的方法,得到了二维高斯波束波形因子在球坐标系中的解析公式.结合广义米理论推导了在轴二维高斯波束入射多层球粒子的电磁散射的解析解,并对散射强度随散射角的分布进行了数值模拟,结果与平面波入射情况进行了比较. 关键词： 矢量波函数 波形因子 电磁散射 广义米理论     

非守恒型粘性流方程的展开方法和数值模拟

在曲线坐标系中，给出了非守恒粘性流矢量方程一种新的展开方法，应用此展开方法使方程的展开式得到简化。对扩压管和二维平面叶栅进行了数值计算，计算结果表明，所给出的新展开式具有实用价值。     

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．     

Relation between the parabolic and spherical eigenfunctions of hydrogen

It is shown that the transformation coefficients relating the eigenfunctions of the Kepler problem in parabolic and spherical coordinates respectively are the normalized Clebsch-Gordan coefficients.     

Acoustic cavity modes in lens-shaped structures

A method for solving exactly the Helmholtz equation in parabolic rotational coordinates is presented using separability of the eigenfunctions and the Frobenius power series expansion technique. Two examples of interest in acoustics are considered and analyzed quasianalytically: The acoustic pressure in a cavity defined by two paraboloids (forming a lens-shaped structure) with (I) rigid wall boundary conditions and (II) pressure-release boundaries. The rigid-wall (pressure-release) acoustic enclosure problem is a Neumann (Dirichlet) boundary condition problem. In both cases, eigenfunctions and eigenmodes are calculated and the shape dependence of the eigenvalue for the ground state is examined.     

Quantum Hamilton--Jacobi Approach to Two Dimensional Singular Oscillator

We obtain the solutions of two-dimensional singular oscillator which is known as the quantum Calogero-Sutherland model both in cartesian and parabolic coordinates within the framework of quantum Hamilton Jacobi formalism. Solvability conditions and eigenfunctions are obtained by using the singularity structures of quantum momentum functions under some conditions. New potentials are generated by using the first two states of singular oscillator for parabolic coordinates.     

External electric field effect on the optical rectification coefficient of an exciton in a spherical parabolic quantum dot

External electric field effects on the optical rectification coefficient of an exciton confined in a spherical parabolic quantum dot are theoretically investigated. To this end, energy eigenvalues and eigenfunctions of the system are calculated, using the direct matrix diagonalization method. The compact-density matrix approach and an iterative method are used to find the optical rectification coefficient of a typical GaAs parabolic quantum dot. The results show that the optical rectification coefficient strongly depends on the confinement frequency and the magnitude of the electric field. Moreover, the peak value of this optical quantity is shifted to the aspect of high energy when the influence of the electric field is considered.     

Transformation Between Eigenfunctions of Three Components of Geometric Momentum on Two-Dimensional Sphere

A technique of coordinate transformation is devised to overcome the computational difficulty associated with the direct transformation between eigenfunctions of three components of the geometric momentum on two-dimensional spherical surface, and the computations are firstly carried out in new coordinates and secondly the results are transformed back into the original coordinates. The eigenfunctions of different components of geometric momentum is explicitly demonstrated to transform under the spatial rotations in the precise way we anticipate.     

Transformation Between Eigenfunctions of Three Components of Geometric Momentum on Two-Dimensional Sphere

A technique of coordinate transformation is devised to overcome the computational difficulty associated with the direct transformation between eigenfunctions of three components of the geometric momentum on two-dimensional spherical surface, and the computations are firstly carried out in new coordinates and secondly the results are transformed back into the original coordinates. The eigenfunctions of different components of geometric momentum is explicitly demonstrated to transform under the spatial rotations in the precise way we anticipate.     

Propagator for a harmonically bound charged particle in a constant magnetic field and with the vector potential of a solenoid

Performing the constrained path integral in polar coordinates, the propagator for a harmonically bound charged particle subjected both to a constant magnetic field and to the vector potential of an infinitely thin solenoid containing magnetic flux is evaluated exactly. The result is then used to derive the energy eigenfunctions, the energy eigenvalues and the Bloch density matrix of the system considered.     

Interbasis expansions for isotropic harmonic oscillator

The exact solutions of the isotropic harmonic oscillator are reviewed in Cartesian, cylindrical polar and spherical coordinates. The problem of interbasis expansions of the eigenfunctions is solved completely. The explicit expansion coefficients of the basis for given coordinates in terms of other two coordinates are presented for lower excited states. Such a property is occurred only for those degenerated states for given principal quantum number n.     

On the quantization of solid body rotation

A general method for solving the problem of quantization of a top is proposed that allows for finding the Hamiltonian eigenfunctions in the form of polynomials of various degree n in the Cartesian coordinates with the use of the Lamé functions. All three coordinates x, y, and z are equivalently involved in computations, as well as their relations with ellipsoidal coordinates, which makes the computations symmetric.     

On the eigenfunctions of the Dirac operator on spheres and real hyperbolic spaces

The eigenfunctions of the Dirac operator on spheres and real hyperbolic spaces of arbitrary dimension are computed by separating variables in geodesic polar coordinates. These eigenfunctions are then used to derive the heat kernel of the iterated Dirac operator on these spaces. They are then studied as cross sections of homogeneous vector bundles, and a group-theoretic derivation of the spinor spherical functions and heat kernel is given based on Harish-Chandra's formula for the radial part of the Casimir operator.