Nuclear Effects in Structure Functions xFa（x, Q^2） from Charge Current Neutrino Deep Inelastic Scattering

By taking advantage of the model-independent nuclear parton distributions, the structure functions xF3（x, Q^2） are calculated, in comparison with the experimental data from CCFR neutrino-nuclei charge current deep inelastic scattering. It is shown that shadowing and anti-shadowing effects occur in valence quark distributions for small and medium x regions, respectively. It is suggested that the neutrino experimental data should be employed in the future for pinning down the nuclear patton distributions.     

金属上化学吸附的族模型量子化学研究

簇模型方法是研究化学吸附的最重要的量子化学方法之一。本文对＇簇－－表面类比法＇的物理内涵、研究现状、以及发展趋势作了简要的评述。     

吡啶团簇的多光子电离和离解研究

利用飞秒激光和飞行时间质谱结合从头计算对吡啶团簇的多光子电离和离解进行了研究. 给出了吡啶团簇的稳定结构和簇内的质子转移过程.     

BRILL－NOETHER MATRIX FOR RANK TWO VECTOR BUNDLES

Lei X be an arbitrary smooth irreducible complex projective curve, E (?) X a rank two vector bundle generated by its sections. The author first represents E as a triple {D1,D2,f}, where D1 , D2 are two effective divisors with d = deg(D1) + deg(D2), and f ∈ H0(X, [D1] |D2) is a collection of polynomials. E is the extension of [D2] by [D1] which is determined by f. By using f and the Brill-Noether matrix of D1 + D2, the author constructs a 2g X d matrix WE whose zero space gives Im{H0(X,[D1]) (?) H0(X, [D1] |D1)}(?)Im{H0(X, E) (?) H0(X,[D2]) (?) H0(X,[D2] |D2)}. From this and H0(X,E) = H0(X, [D1]) (?) Im{H0(X, E) (?) H0(X, [D2])}, it is got in particular that dimH0(X, E) = deg(E) - rank(WE) + 2.     

A Comparison of Different Measures for Dynamical Event Mean Transverse Momentum Fluctuation

Various measures for the dynamical event mean transverse momentum fluctuation are compared with the real dynamical fluctuation using a Monte Carlo model. The variance calculated from the G-moments can reproduce the dynamical variance well, while those obtained by subtraction procedures are approximate measures for not very low multiplicity. Фpt, proposed by Gadzicki M and Mrowczynski S [Z. Phys. C 54 (1992)127], can also serve as an approximate measure after being divided by the square root of mean multiplicity.     

TC2模型与轻子味破坏过程l_i→l_jν_l_l

许多超出标准模型的新物理预言了非普适规范玻色子Z′的存在 .此粒子可产生许多新物理现象 .本文计算了顶色辅助的人工色 (TC2 )模型预言的非普适规范玻色子Z′对轻子味破坏 (LFV)衰变过程li→ljνl νl 的贡献 .结果表明 ,在整个参数空间内 ,过程τ± →ljντ ντ 的分支比比τ± →ljνl νl(l =μ ,e)的分支比大得多 .考虑实验测量值上限Brexp(μ→ 3e)≤ 1× 10 -12 对TC2模型的自由参数的限制 ,我们给出了一些轻子味破坏过程的上限 .在大部分参数空间中 ,分支比Br(τ± →ljντ ντ)～ 10 -6,Br(τ± →ljνl νl)～ 10 -9.这些结果可以用来部分地解释中微子振荡数据 ,将来的高能实验有可能探测到此新物理效应 .     

快速多极边界元法解的存在唯一性

本对求解3维弹性摩擦接触问题的快速多极边界元法(FM—BEM)在数学理论上作了深入探讨．首先，利用向量和子空间理论找出快速优化广义极小残余算法(GMRES(m))求解边界元方程组所满足的代数条件．使对工程用FM—BEM解的研究转化为对代数问题的讨论，然后．分三步证明了FM-BEM解的存在唯一性，为FM-BEM求解弹性摩擦接触工程问题提供强有力的数学支撑．     

稳定的不变子空间的扰动界限

§1.引言 1.1.稳定的不变子空间 在矩阵的各类不变子空间中,从扰动分析的角度研究得比较深入的,是由根子空间的直和构成的不变子空间。     

球约束凸二次规划的一个新算法

首先利用Lagrange对偶 ,将球约束凸二次规划问题转化为无约束优化问题 ,然后运用单纯形法求解无约束优化问题 ,从而获得原问题的最优解