利用高频结构仿真器分析波导魔T

高频结构仿真器（HFSS）是一种微波器件设计软件，该软件界面友好，通过仿真计算减小了调试工作量，使得微波器件的设计变得简单易行。本文利用HFSS对波导魔T进行了仿真分析，得到了该器件的S参数和动、静态场的分布情况，并对该器件进行了优化设计。     

碳纳米管的场发射特性

研究了碳纳米管的场致发射特性，实验证明碳纳米管作为场发射阴极材料具有优越性。通过对碳纳米管进行温度处理，得到了与基片附着力强的碳纳米管；测试了场发射特性，发现碳纳米管其开启电压较低(30V)。     

阵列天线的源场测试法

本文论述了基于源场法的阵列天线测试原理，给出了用该方法下的测试结果和远场法的测试结果，并对这两种方法测得的结果进行了简要分析。     

场顺序彩色显示器

荫罩CRT受自身结构的限制,要进一步改进其分辨率就有很大的困难。近年已研制成一种获得彩色图像的颇有吸引力的替代品,即场顺序彩色显示器。它由单色CRT和液晶电子色闸组成,称之为LC/CRT系统。液晶电子色闸由液晶π盒及其连用的偏振片组成,可看成是老式机械彩色轮那样的一种电控色带带通滤色片。本文描述了液晶电子色闸的功能及其工作优点,讨论了其可能结构与显示特性。     

油水两液相一维非等温渗流的传递分析

在求解油水两液相非等温渗流的温度场、压力场基础上,以驱动功、驱动功率、驱动阻力、驱动速率为特征参数,对该过程进行(火用)传递分析。数值模拟的结果表明:含水通过降低油的相对渗透率、从而增大驱动阻力、减小驱动功率, 最终导致原油产量降低。     

赤道不是轨道弧的n次多项式向量场的Poincaré紧化场之拓扑结构

本文证明了赤道不是轨道弧的n次多项式向量场的Poincare紧化场之拓扑结构包含赤道是轨道弧的n-1次多项式向量场的Poincare紧化场之拓扑结构;当n=2时,这种包含关系是相等的,且其Poincare紧化场有五种不同的拓扑结构;当n=2k+1(k=1,2…)时,这种包含关系是真子集。     

Measurement of the Seperation between Atoms beyond Diffraction Limit

We propose a scheme to obtain the distance of two identical atoms placed inside the standing wave field by monitoring the collective resonance fluorescence spectrum emitted by the two particles. We find three different parameter ranges, depending on the distance of the atoms as compared to the transition wavelength. For large interparticle distances, dipole-dipole coupling is negligible, and the main system evolution arises from the interaction with the standing wave field. In the small-distance limit, the dynamics is dominated by the dipole-dipole interaction. Finally, in the intermediate region, a rich interplay of the various couplings arises, which however is lifted for strong driving laser fields. The present measurement procedure allows us to distinguish the three cases. In each of the cases, we show how to determine the distance of the two particles and their respective positions relative to the nodes of the standing wave field with fractional-wavelength precision.     

A Reliability Analysis of Calculated Results for Odd-Even and Odd-Odd Nuclei in Relativistic Mean-Field Theory

We calculate the binding energies of Ni, Cu, Xe, Cs, Pt, Au, Np, Pu isotope chains using two interaction parameter sets NL-3 and NL-Z, and compared the relative errors of the even-even nuclei with those of odd-even nuclei and odd-odd nuclei. We find that the errors of binding energy of odd-even and odd-odd nuclei are not bigger than the one of even-even nuclei. The result shows that comparing with even-even nuclei, there is no systematic error and approximation in the calculations of the binding energy of odd-even and odd-odd nuclei with relativistic mean-field theory. In addition, the result is explained theoretically.