竹子的力学特性

本文用材料力学原理阐述竹子具有的强度及稳定性，用途极广     

氦,氢,氮空心阴极放电的真空紫外辐射特性

介绍了一种水冷、陶瓷封接结构的空心阴极放电装置.研究了He、H_2、N_2在120nm～20Onm范围内该装置的真空紫外辐射特性,获得了100～600mA电流范围内的辐射强度与放电电流的关系,以及充气气压变化对它的影响.实验表明:在实验条件下,主要发射谱线为氮的原子线和氦的离子线;辐射谱线强度在0.03～0.72mW·cm~(-2);气压改变时,N_2、H_2辐射强度有一极大值,而He的离子线辐射强度则出现二个极大;在He/H_2混合气体放电时,随着He的加入,氢分子带光谱有明显下降.     

激光合作目标用玻璃微珠的研制

本文研究了玻璃及成珠工艺对激光合作目标特性的影响，并设计了特殊设备和工艺规程，在此基础上研制出高性能激光合作目标用的玻璃微珠     

N2���������ŵ���΢���������ŵ�ת���PIC/MCģ��

开发了氮空心阴极放电PIC/MC二维自洽模型。研究了N2传统空心阴极向微空心阴极放电转变过程中电势和电场的变化。结果表明,不同尺寸的空心阴极放电的电势及电场分布规律几乎类似,但空心阴极孔径减小且气压增加时,电场近似线性增加;典型微空心阴极电场比传统空心阴极放电电场约大3个量级;微空心阴极放电产生的电子,氮分子离子和氮原子离子的密度比传统空心阴极放电约大3个量级,且微空心阴极放电中,N2+密度比N+密度大8倍以上。     

New Expressions for Dark-Hollow Light Beams

A class of new light beams of dark-hollow beams, named sinusoidal dark-hollow beams, is introduced. The propagation formula for a sinusoidal dark-hollow beam through a paraxial ABCD optical system is derived. The propagation properties of the sinusoidal dark-hollow beam are comparatively studied and illustrated with numerical examples.     

N2/Ti微空心阴极放电等离子体阴极溅射模拟

采用Monte Carlo方法模拟N2/Ti微空心阴极放电等离子体阴极溅射过程,其中,氮离子(N2+,N+)轰击阴极表面采用PIC/MC模型模拟.计算溅射钛原子的热化过程、钛原子的密度及其平均能量分布.结果表明,沿各方向溅射出的90%金属Ti原子所带的初始能量小于30 eV,其散射角主要分布在30°和60°之间;溅射Ti原子在离微空心阴极壁约0.04 mm处出现热化极大值.     

掺钛空心玻璃微球制备技术

为实现惯性约束聚变靶用空心玻璃微球的均匀掺杂,采用溶胶-凝胶技术结合炉内成球法,以钛酸四丁酯为掺杂剂,对钛掺杂玻璃溶胶-钛掺杂玻璃凝胶-钛掺杂干凝胶粒子-钛掺杂空心玻璃微球（Ti-HGM）这一掺钛空心玻璃微球的制备方法进行了探索。实验结果表明:掺钛效应使空心玻璃微球壁厚均匀性、同心度有所降低,但对壁厚、直径控制基本无影响;Ti与Si原子分数比为2.23%的Ti-HGM掺杂基本均匀,近70%微球的保气半寿命在一个月以上。     

Determinations of plasma density and decay time in the hollow cathode discharge by microwave transmission

The microwave （MW） transmission method is employed to measure both the plasma density and the plasma decay time in the hollow cathode discharge （HCD） in argon at low pressure. The plasma density in DC-driven or pulsed HCD is on the order of 1012 cm-3, which can block the X-band MW effectively. In the case of pulsed HCD, the MW transmittance shows the same waveform as the pulsed current during the rising edge if the driving frequency is low, but with a longer delay during the falling edge. The MW transmittance reaches a constant low level when the driving frequency is high enough. The plasma decay time in the HCD system is measured to be about 100 μs around a pressure of 120 Pa. The ambipolar diffusion is considered to be the major mechanism in the decay process.