外加磁场对碰撞射频鞘层离子能量分布的影响

采用双流体模型,数值研究入射到射频鞘层偏压电极上的离子能量分布.研究结果表明：磁场在改变离子运动状态的同时,调控着基板上的离子能量分布,使之在垂直基板方向和平行基板方向间转移. 关键词： 等离子体 射频 鞘层 磁场     

The p–T phase diagram of KNbO3 by a dielectric constant measurement

A dielectric constant measurement was carried out on perovskite-type ferroelectrics KNbO₃ over a wide range of temperature under high pressure. The temperature- and pressure-dependence of the dielectric constant clarified that all temperatures of the transitions from the ferroelectric rhombohedral to orthorhombic, to tetragonal and then to the paraelectric cubic phase, decrease with increasing pressure. These results indicate that the orthorhombic–tetragonal transition takes place at 8.5 GPa and the tetragonal–cubic transition at 11 GPa, at room temperature.     

Study of N*(1440) from J/Ψ decays

For J/Ψ↦ pπ⁰ and pπ⁺π^-, the π⁰ p and pπ⁺π^- systems are limited to be pure isospin-(1/2) due to isospin conservation. This is a big advantage in studying N^* resonances from J/Ψ decays, compared with πN and γN experiments. The process J/Ψ↦ N ^* or p provides a new way to probe the internal structure of the N^* resonances. Here we report a quark model calculation for J/Ψ↦ p, N ^*(1440) and N ^*. The implication for the internal structure of N ^*(1440) is discussed. Received: 1 June 2001 / Accepted: 20 June 2001     

Baryon rapidity loss in relativistic Au + Au collisions

An excitation function of proton rapidity distributions for different centralities is reported from AGS Experiment E917 for Au+Au collisions at 6, 8, and 10.8 GeV/nucleon. The rapidity distributions from peripheral collisions have a valley at midrapidity which smoothly change to distributions that display a broad peak at midrapidity for central collisions. The mean rapidity loss increases with increasing beam energy, whereas the fraction of protons consistent with isotropic emission from a stationary source at midrapidity decreases with increasing beam energy. The data suggest that the stopping is substantially less than complete at these energies.     

基于分子表面静电势参数分析溶剂的极性性质

用理论教育处导出的分子表面静电势参数II和σ^2tot对一系列溶剂的五种极性 批E^N T、π^*、Py、SPP和S‘进行了相关分析,与Catalan的理论热力分析结果进行了比较。结果显示：S‘是一个适用性委有好的溶剂极性参数,而质子性溶剂的E ^NT值、芳香化合物和多卤代化合物的π ^*值和SPP值则存在着一定的非极性因素。     

电流变液成链过程的一种序参量描述

A simple long-range-order parameterPis defined for describing the process of formation of chains in the electric field direction. The free energy of the system is taken to be the sum of the internal energy, the electrostatic interaction and configuration entropy as a function o P. Calculated results indicate that the critical parameter is a function of electric field, temperature, misfit dielectric coefficients and concentration of particles.     

掺锡As2S8薄膜光折变效应及其在条波导制备中的应用研究

实验研究了Sn₁As₂₀S₇₉非晶态半导体薄膜的光折变效应及其膜厚变化的现象,归纳了沉积态样品、退火态样品和光饱和态样品的实验规律,提出和采用紫外光激励的方法试制了Sn₁As₂₀S₇₉条形波导,632.8 nm波长导模激励显示该波导具有良好的导波特性. 关键词： 光波导技术 硫属化合物玻璃 光阻断效应 光折变效应     

用于POF的高性能共振腔发光二极管

提出用AlGaAs材料为n型下DBR,AlGaInP材料为p型上DBR,GaInP/AlGaInP多量子阱为有源区来制备650nm波长的共振腔发光二极管（RCLED）.用传输矩阵法对器件的结构进行了理论设计,并制备了RCLED和普通LED两种结构.测试结果表明,RCLED有更高的发光效率,是普通LED的近1.3倍,当注入电流从3mA增加到30mA时,RCLED的峰值波长只变化了1nm,而普通LED的波长则变化了7nm,且RCLED的光谱半宽窄,远场发散角小. 关键词： 发光二极管 共振腔 金属有机物化学气相淀积     

Adaptive Laser Aiming Through 2 km Horizontal Atmosphere with Precise-Delayed SPGD Algorithm

Journal of Russian Laser Research - Laser aiming is one of the key technologies of laser atmospheric transmission. The beam actually is affected by atmospheric turbulence and mechanical vibration;...     

气体团簇离子束两步能量修形法的平坦化效应

本文提出采用气体团簇离子束的两步能量修形法来改善4H-SiC(1000)晶片表面形貌.先用15 keV的高能Ar团簇离子进行整体修形,再用5 keV的低能团簇离子优化表面.结果表明,在相同的团簇离子剂量下,与单一15 keV的高能团簇处理相比,两步法修形后的表面具有更低的均方根粗糙度,两者分别为1.05 nm和0.78 nm.本文还以原子级平坦表面为研究对象,揭示了载能团簇引起的半球形离子损伤(弧坑)与团簇能量的关系,及两步能量修形法在弧坑修复中的优势.在原子力显微镜表征的基础上,引入了二维功率谱密度函数,以直观全面地给出材料的表面形貌特征及其随波长(频率)的分布.结果表明,经任何能量的团簇离子轰击的表面,在0.05—0.20μm波长范围内,团簇轰击都能有效地降低粗糙度,而在0.02—0.05μm范围内,则出现了粗化效应,这是由于形成了半球形离子损伤,但第二步更低能量的团簇离子处理可以削弱这种粗化效应.