DISTRIBUTION OF THE（0，∞）ACCUMULATIVE LINES OF MEROMORPHIC FUNCTIONS

Suppose that f(z)is a meromorphic function of order λ（0<λ<+∞）and of lower order μ in the plane.Let ρ be a positive number such that μ≤ρ≤λ.(1)If f^(l)(z)(0≤l<+∞）has p(1≤p<+∞）finite nonzero deficient valnes αi(i=1,…，p)with deficiencies δ（αi,f^(l)),then f(z)has a (0,∞）accumulative line of order ≥ρin any angular domain whose vertex is at the origin and whose magnitude is larger than max(π/ρ，2π-4/ρ ∑i=1^p arcsin √δ（αi,f^(l))/2).(2)If f(z) has only p(0<p<+∞）（0,∞）,accumulative lines of order≥ρ：arg z=θk(0≤θ1<θ2<…<θp<2π，θp+1=θ1+2π）,then λ≤π/ω，where ω=min I≤k≤p(θk+1-θk),provided that f^(l)(z)(0≤l<+∞）has a finite nonzero deficient value.     

特殊向量丛的存在定理

本文给出紧 Riemann 曲面上特殊不可分解向量丛的一个存在定理和特殊单向量丛、特殊稳定向量丛存在假设的一个反例及2维特殊稳定向量丛的一个存在定理.     

带有不等式约束的全局最优性条件

本文利用不连续罚函数方法将带有不等式约束的全局优化问题的求解转化为 讨论一非线性方程的求根问题,从而得到若干个全局最优性条件.     

绝对连续测度的Loeb代数

It is proved that if μ and v be finite measures on a measurable space (X,S) and v is absolutely continuous with respect to v, then it is holds that L(^*S,^*v) C L(^*S,^*v), while L(^*S,^*v) and L(^*S,^*v) are the Loeb algebras with respect to measure spaces (X,S,μ) and(X,S,μ).     

纬向对称准地转流的非线性稳定性定理

建立了周期域上准地转流在一般的边界条件下对应于Arnold第二定理的非线性稳定性定理。将扰动能量与扰动拟能的上界用初始扰动场的显示表示出来，从而建立了Liapunov意义下的非线性稳定性定理。     

关于Fejer点上的一种复有理型插值的一致逼近阶

设D是一个Jordan,Г为其边界，并设Г满足Aльпер条件。本文得到了一种基于Fejer点的有理型插值算子对于f(z)∈C（Г）的一致逼近阶。     

稠密等离子体的含温有界超Hartree-Fock自洽场原子结构

研究等离子体辐射不透明度和状态方程的核心问题是原子结构计算问题。平均原子一直是主流模型，但有缺陷：电子交换势一直停留在Fermi—Dirac统计基础上；自由电子与束缚电子的划分采用了经典判据；电子间的自作用和自交换作用难以真正抵消；给出的能级、电子占据数、化学势特别是基态能量，很不准确。如果温度持续降低，等离子体应逐渐凝聚成固态物质，平均原子应过渡到真实原子。而绝大多数平均原子模型都无法作到这一点。要精确计算等离子体内的原子结构参数，必须使用具有很高精度的Hartree-Fock自洽场原子结构模式。     

n维氢原子的散射态

研究了n维氢原子的散射态性质．给出了精确的按“k/2π标度”归一化的散射态的精确解波函数及相移表达式，讨论了相移的解析性质，获得了束缚-连续跃迁矩阵元的解析计算公式．普通氢原子(n=3)散射态的有关结果作为特例包含在本文的一般结论之中． 关键词： n维氢原子 散射态 精确解 相移 束缚-连续跃迁矩阵元     

关于Lipschitz区域上Schr(o..)dinger方程的不连续边界值问题

讨论Lipschitz区域上Schrodinger方程的不连续边界值问题及其研究进展,给出Lp(p＞1)边值问题和Hp(p＜1)边值问题的位势理论.同时指出Besov-Sobolev边值、Orlicz边值等需要进一步研究的问题.     

Langevin Simulation of Non-Uniform Granular Gases

We present and study a fractal model of a non-uniform granular system for the first time, based on which wenumerically solve the dynamics actions in the system successfully in one-dimensional case. The multi-mixture is composed of N different particles, whose granularity distribution has the fractal characteristic. The particles are subject to inelastic mutual collisions and obey to Langevin equation between collisions. Far from the equilibrium,i.e. the given typical relaxation time τ of the driving Brownian process is much larger than the mean collision time τc, the results of simulation indicate that the degree of inhomogeneity in the granularity distribution signed by the fractal dimension D of size distribution has great influence on the dynamics actions of the system. The velocity distribution deviates obviously from the Gaussian distribution and the particles cluster more pronouncedly with the larger value of D in the system. The velocity distribution and spatial clnsterization change with D are presented.