氯化三有机基锡和氯化三有机基铅与三苯基氧胂配合物的合成和晶体结构研究

描述了一事三苯基氧胂Ｐｈ３ＡｓＯ．Ｈ２Ｏ（１）及其与氯化三苯基锡,氯化三对氯苯基锡及氯化三苯基铅配合物「Ｐｈ３ＳｎＣｌ（ＯＡｓＰｈ３）」（２）,「（ＣｌＰｈ）３ＳｎＣｌ（ＯＡｓＰＨ３）」（３）和」Ｐｈ３ＰｂＣｌ（ＯＡｓＰｈ３）（４）的合成和晶体结构,晶体数据分别为（１）单斜晶系,空间群Ｐ２、／ｎ,ａ＝９．４６０４（７）,ｂ＝１６．６３４７（７）,ｃ＝１１．１５４４（１１）Ａ,Ｂ＝１１３．２３３（６     

A Lattice Model for Bidirectional Pedestrian Flow on Gradient Road

Ramps and sloping roads appear everywhere in the built environment. It is obvious that the movement pattern of people in the sloping path may be different as compared with the pattern on level roads. Previously, most of the studies, especially the mathematical and simulation models, on pedestrian movement consider the flow at level routes. This study proposes a new lattice model for bidirectional pedestrian flow on gradient road. The stability condition is obtained by using linear stability theory. The nonlinear analysis method is employed to derive the modified Korteweg-de Vries (mKdV) equation, and the space of pedestrian flow is divided into three regions: the stable region, the metastable region, and the unstable region respectively. Furthermore, the time-dependent Ginzburg—Landan (TDGL) equation is deduced and solved through the reductive perturbation method. Finally, we present detailed results obtained from the model, and it is found that the stability of the model is enhanced in uphill situation while reduced in downhill situation with increasing slope.     

μ介子寿命与μ-e对称性的实验限度

μ介子有反常作用,破坏了μ-e对称性。本文讨论了反常作用对弱作用过程的影响,分析了反常作用的电荷无关性和r₅变换性质与μ蜕变弱作用常数的重正化之间的联系,证明了重正化后G_V=G,G_A=εG,ε=1+δ。利用这一结果,可以解释矢量流守恒假定下普适V-A费米弱作用理论在解释μ介子寿命时遇到的困难。从理论和实验的比较中定出δ=0.04,这是由μ蜕变定出的μ-e对称性的实验限度。     

动量为6.8BeV/cπ-介子与核子的非弹性作用

本工作共积累了317个非弹性作用事例。作用中的次级带电粒子在(π^--N)质心系中的角分布与动量分布等和前人结果一致,并且基本上可以用边缘碰撞机制来说明。对带有次级质子的事例作了如下分析:(1)计算全部次级粒子(质子除外)在它们自己系统中的总能量ω。作ω分布,并与边缘碰撞1π交换近似计算的理论曲线比较,在ω=1.5BeV附近观察到有突出于理论曲线之外的高峯,并对峯区内事例进行了初步分析。(2)综合我们的和联合原子核研究所的数据,计算了次级质子在镜象系的非弹性系数K_з,并使K_з值的分布与根据Барашенков等人理论计算的K_з分布曲线作了比较。此外,还试从靶质量观点出发,利用Duller-Walker的F图方法,对不同K_з值的各类事例进行了分析和讨论。     

General self-dual non-abelian plane waves

Yang's R-gauge formulation is used to obtain the most general self-dual non-abelian plane wave solutions.