两指标点过程的停止及σ-域

本文给出两指标点过程的跳线刻划、停止方法,论述了跳线的可测性及点过程有关的σ-域的结构和特征。     

一个改进的Reissner-Mindlin矩形元

本文提出了一个改进的Reissner-Mindlin矩形非协调元方法：旋度用连续双线性元逼近，横向位移用旋转矩形非协调元逼近，而作为中间变量的剪切力用增广的分片常数元逼近，我们证明：该方法具有关于板厚一致稳定性和一致最优收敛性。     

Ultrafast carrier dynamics in purified and as-grown single-walled carbon nanotube films

Ultrafast time-resolved optical transmissions in purified and as-grown single-walled carbon nanotube films are measured at a temperature of 200K. The signal of the purified sample shows a crossover from photobleaching to photoabsorption. The former and the latter are interpreted as the state filling and the red shift of the π-plasmon, respectively. The signal of the as-grown sample can be perfectly fitted by a single-exponential with a time constant of 232fs. The disappearance of the negative component in the as-grown sample is attributed to the charge transfer between the semiconducting nanotubes and the impurities.     

直线感应加速器加速腔物理设计与研究

简要介绍直线感应加速器（ＬＩＡ）加速腔物理设计的几个关键问题．讨论了加速电压及其平顶和腔参数的关系．对腔的耦合阻抗与束流不稳定性的关系作了概念性介绍，分析了降低耦合阻抗的途径．并给出两个加速腔设计原型．     

BALLOONING INSTABILITY IN HIGH β TOKAMAK

In this paper we show that Δ′_B is negative over parts of the second region, and that plasmas are stable to Δ′_B-driven resistive modes for realistic equilibria in which characteristics of finite-β configurations are retained. We have found that ideal instability is very sensitive to the ratio T=rΔ″/Δ′ in the second region. In comparison with previous works. results obtained by present authors show that the shift gradient Δ′ has a significant stabilizing effect on the second stable boundary, and this effect increases as the shear s becomes larger.     

用解几方法解某些立几题

本文试图通过几个例子介绍一下用平面解析几何方法处理某些立体几何问题。 例1在直角坐标系内有互不重合的四点A、B、C、D,其坐标分别为(x:,g,)、(勺,烧)、 (心,骊)、(x’,如).,且A、e和B、D在x轴的两旁,将这平面沿x轴折成二面角后,求过A、B的直线与过C、D的直线共面的条件。 解:设这四点的位置如图一,若它们共面,则有:l)直线AC与BD都交x轴于同一点尸,设坐标 为(a,o).于是有::月材上!尸N!2 因此,的椭圆;了. 例3材N,…}了协f 12+}MN!“=了,即尸·sin26+了=矛. 当。<6<合时,所求轨迹为上式所表示当。=令时,所求轨迹为一个圆尸+犷=,已…     

LIA加速腔物理设计与实验检测

简要介绍了直线感应加速器（ＬＩＡ）加速腔物理设计和实验检测的几个关键问题，讨论了加速电压及其平顶和腔参数的关系。对腔的耦合阻抗与束流不稳定性间的关系作了概念性介绍，分析了降低腔耦合阻抗的途径。最后，概略说明了加速腔主要设计性能的实验检测技术。     

理想的分形模型和实际的嵌套结构

自然界中的分形结构与理想的分形模型不同，它的自相似性只在统计意义上和有限的尺寸范围内成立。材料中，在一个大尺寸范围内的不同度域可以存在不同的分形结构，形成多度域分形。材料的性能与分形结构的上下界限密切相关，因此在研究性能与分形的关系时，首先要找准哪一个分形结构与所研究的性能相关。另外，用Ｍａｎｄｅｌｂｒｏｔ的周界－面积关系来测分维时，因受到一定条件的约束而不太方便，建议用周长－最大直径法来测分维。     

Temperature－Induced Switching－Over of the Luminescence Transitions in GaInNAs／GaAs Quantum Wells

Photoluminescence (PL) spectra of the GaInNAs/GaAs single quantum well (SQW) with different N compositions are carefully studied in a range of temperatures and excitation power densities. The anomalous S-shape temperature dependence of the PL peak is analysed based on the competition and switching-over between the peaks related to N-induced localized states and the peak related to interband excitonic recombination. It is found that with increasing N composition, the localized energy increases and the turning point of the S-shape temperature dependence occurs at higher temperature, where the localized carriers in the handrail states obtain enough thermal activation energy to be dissociated and delocalized. The rapid thermal annealing (RTA)effectively reduces the localized energy and causes a decrease of the switching-over temperature.     

里德堡(Rydberg)原子

“里德堡原子”在文献中出现,只是近四、五年的事。随着原子物理理论与实验手段的进一步发展,对里德堡原子的研究越来越引起人们的注意,它已成为原子物理学一个必不可少的分支。 一、里德堡原子的结构和能级 原子体系的能量其主要部分是由主量子数n决定的(无论是简并或非简并情况)。高激发态原子,就称做里德堡原子。它的主量子数n,高达几十以至上百。自然界中处于这样高的激发态原子数目不多,主量子数n一般是几十。 对于处在高激发状态的氢原子即里德堡氢原子,玻尔(Bohr)氢原子模型给出了一个很好的近似。虽然这时主量子数n很大,原子核外部…