多尺度模拟与计算研究进展

简要介绍了多尺问题与研究方法.重点论述了两类常见多尺度问题的模拟计算方法与研究进展,分析了各自的优缺点和使用范围.对现有研究的局限性和存在的问题进行分析,指出了进一步研究多尺度模拟与计算的必要性.介绍了求解含有孤立缺陷问题的非局部准连续体法,MAAD等方法以及求解基于微观模型本构模拟问题的局部连续体法、HMM等方法.文章对多尺度模拟与计算的前景进行展望,提出了一些亟待解决的问题.     

根值判别法的两个推广

讨论正项级数的根值判别法．若将判别极限lim↓n→∞ n√an更改为lim↓n→∞或lim↓n→∞^n√am^n＋i,则相应结果在一定条件下将比原判别方法更为精细,且应用范围也有所推广．     

动态水声环境不确定性的预报与估计

水声环境具有强烈的时空易变性,为了解其变化中的规律和产生的不确定性,将POM海洋数值模型和水声传播模型FOR3D进行耦合,建立海洋—声学耦合数值模式。对海区的温盐等环境参数和水下声场进行预报,给出了典型断面的温度垂直结构、实验海区声速剖面和传播损失。同时,采用集合卡尔曼滤波(EnKF)方法结合海洋—声学耦合数值模式分析了水声环境的不确定性,对不同深度与频率下,传播损失的均值与满足90%的可能区间进行了计算,同时给出了不同点声速、传播损失、声纳作用距离的不确定性直方图。和实验数据的对比结果表明该方法具有较高的有效性,能对水声环境的不确定性进行合理的预报与估计。     

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。     

3C-SiC纳米颗粒量子限制效应的实验证据

报道了关于3C—SiC纳米颗粒量子限制效应的实验证据．将电化学腐蚀3C—SiC多晶靶材得到的多孔材料在水溶液中进行超声处理，制备出发光的3C—SiC纳米颗粒溶液．透射电镜实验表明，所得颗粒直径分布在1-6nm范围，光致发光谱实验给出了存在量子限制效应的实验证据．发光范围在440-460nm．SiC纳米颗粒量子限制效应的发现，为该材料在光电子发光器件中的应用提供了重要的实验基础．     

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.