Measurement of Titanium and Manganese K -shell Ionization Cross Sections by Electron Impact

报道了电子引起的钛、锰原子的Ｋ壳层电离截面实验值。实验中,采用了薄靶厚衬底技术,并将衬底中反射的电子对测量值的影响进行了修正。实验结果与其他文献报道的测量结果相吻合。最后,还将实验结果与Ｃａｓｎａｔｉ等人的经验公式进行了比较。     

用椭偏术研究与接触介质有关的贵金属的介电函数

为了研究接触介质对金属光学性质的影响，实验中使用具有不同折射率的梯形棱镜作为衬底，将金和银蒸发到棱镜底部，用椭偏术分别测量了薄膜在金属-空气、金属-衬底界面的介电函数.结果表明：无论在Drude区，还是在带间跃迁区，金属-衬底界面处薄膜介电函数不仅与金属-空气界面处的测量值不同，而且随衬底折射率改变而改变.在固体接触条件下获得的结果与其他作者在液体接触条件下获得的结果相一致，但尚难被现有机制所解释. 关键词：     

硅化物薄膜的质子弹性散射分析

本文报道了一种分析硅衬底上SiN_x和SiO_x的N/Si和O/Si含量比的简便方法。用1.95MeV质子弹性散射测量薄膜(9000—15000)的组分比和厚度,实验值与2.1MeVHe的背散射分析(RBS)结果符合得很好;对微米以上厚度样品,MeVH束分析更为有利,这是与He束背散射分析互补的一种方法。文中给出了实验结果,并进行了讨论。 关键词：     

模折射率透镜的研制

本文报道在K7玻璃衬底上制作光波导模折射率透镜的实验结果,包括透镜的设计、制备及性能的测量。     

一种测量功率型LED热阻的方法

叙述了正向电压法测量功率型LED温度系数K和热阻的原理,介绍了测试装置及具体测试过程,对蓝宝石衬底正装LED和硅衬底倒装LED的温度系数和热阻进行了测量.选用热阻已知的LED样品,对其实际值与测量值进行了比较,误差在5% 左右,证实了这种热阻测量方法是可行的.     

棱镜耦合法测波导衬底折射率

本文对棱镜耦合法测波导衬底折射率进行了实验研究,在两种入射情况下,对石英玻璃、CaF_2、LiF衬底及C-813-8胶块进行了折射率测量,并得到有益的实验结果.     

磁控溅射CNx薄膜的附着力、粗糙度与衬底偏压的关系

对磁控溅射生长在单晶Si(001)衬底上的CNx薄膜的附着力、粗糙度与衬底偏压的关系进行了研究。CNx薄膜沉积实验在纯N2的环境下进行．衬底温度(Ts)保持在350℃．衬底偏压(Vb)在0～-150V之间变化。利用原子力显微镜(AFM)和划痕试验机来测量CNx薄膜的表面粗糙度及对衬底的附着力。AFM和划痕实验的结果显示衬底偏压Vb对CNx薄膜的附着力和表面粗糙程度的影响很大，在-100V偏压下生长的CNx薄膜表面最光滑(粗糙度最小)，同时对Si(001)衬底的附着力最好。最后根据实验结果确定了在单晶Si(001)衬底上生长光滑而且附着力好的CNx薄膜的最佳实验条件。     

利用压电光声光谱测量镁掺杂氧化锌薄膜的光吸收特性

采用由射频磁控溅射方法在玻璃衬底制备的镁掺杂氧化锌（ZnO：Mg）薄膜材料,通过压电光声光谱法测量其在可见光波段的光吸收特性,并与透射光谱法测得的吸收率数据进行了比较,得到了一致性较好的结果。同时,从理论上推导分析了玻璃衬底上ZnO：Mg压电光声信号与光吸收率的关系及变化规律,并由实验证实：光声信号为玻璃基底与ZnO：Mg薄膜的共同贡献,光声信号的幅值与吸收率呈反相关,这一结论与理论分析得到的结果一致。     

高温超导YBCO带材的交流传输电流损耗测量

文中对不同频率不同幅值的交变电流下高温超导体YBCO带材的交流传输损耗进行了实验研究。实验在77K下,对Superpower公司生产的SCS4050型号带材采用电测法通过锁相放大器进行了交流损耗值的测量,并将其工作电流为50Hz时的测量结果与Norris矩形模型估算值进行了对比,同时也给出了15Hz到300Hz不同频率下交流损耗测量结果的比较分析。     

高纯区熔单晶硅高增益光晶体管的研究

区熔单晶硅与直拉单晶硅以及其他半导体材料相比杂质含量少,少子寿命长,所以以区熔单晶硅为衬底制作的光晶体管在弱的光信号下仍然有高的增益,适宜于弱光探测.报道了以区熔单晶硅为衬底的光晶体管的实验结果.为了保持区熔高纯单晶硅内的少子寿命,背面淀积了一层掺磷多晶硅作为外吸杂层.已经测量得到对于实验中发射极直径为2mm的光晶体管在波长为0.83 μm的入射光照射下,光功率低至0.16 nW时,光晶体管的增益仍然高达4400.     

Al,Ti,Cu,Mo原子的K壳层电离截面的理论计算

 电子离子碰撞过程是模拟激光等离子体的超热电子的能谱和产额的主要过程之一。基于相对论性的电子离子碰撞的K壳层的电离截面理论,计算了Al,Ti,Cu,Mo原子的K壳层的电子离子碰撞截面,结果和最近的文献实验数值和其它理论数值进行了比较,计算结果可用来模拟激光等离子体的超热电子能谱和产额。     

1.0 MeV电子碰撞引起Ta 和Au 内壳电离截面的测量

无论对深入理解电子-原子的作用机制,还是在材料等领域的实际应用,电子轰击原子的内壳电离截面都具有重要意义。当前电子碰撞引起原子内壳电离的实验数据多集中在几十keV 入射能量和中小Z 靶原子,其它数据相对比较缺乏。本工作以能量为1.0 MeV电子轰击Ta 和Au 靶,通过测量靶原子特征X射线的产额,获得其K壳电离截面分别为13.3 和10.1 b,L 壳电离截面分别为554 和338 b。并将实验结果和相应的理论进行了对比,结果显示,本实验测得的K壳电离截面与Casnati、Hombourger 理论值、L 壳电离截面与Scoeld和Born-Bethe 的理论值相符。Accurate experimental data for atomic inner-shell ionization cross-sections by electrons are of basic importance both in understanding inelastic electron-atom interaction and its application. Up to now, most of available data on this process were mainly concentrated on the low and medium Z atoms by the bombardment of low energy electrons. In present experiments K-shell and L-shell ionization cross-sections of Ta and Au in collisions with 1.0 MeV eleltron were determined by measuring the characteristic X-rays emitted from the target atoms. For the present collision systems the K-shell ionization cross-sections were found to be 13.3 and 10.1 b,and the L-shell ionization cross sections were 554 and 338 b, respectively. The measured K-shell ionization cross sections are in reasonable agreement with the theoretic predictions of Casnati and Hombourger, while L-shell ionization cross sections are consistent with the theoretical results of Soc eld and Born-Bethey.     

K-SHELL IONIZATION OF IRON BY ELECTRON BOMBARDMENT

K-shell ionization cross sections for Fe by electron impact were measured by detecting the characteristic X-rays emitted from the thin solid film target of known mass thickness with a Si(Li) detector. Reflection correction of the substrate was done using a bipartition model of electron transport. The experimental results are satisfactory as compared with the theoretical calculation and empirical formula.     

Mn and Cu K-shell ionization cross sections by slow electron impact

Near the threshold energy, electron induced Mn and Cu K-shell ionization cross sections have been measured. Except for energies very close to threshold, the results are in good agreement with the semi-empirical formula of Green and Cosslett.     

Measurements of K-shell ionization cross sections of35Br,37Rb,39Y using low energy protons

K-shell ionization cross section measurements are reported for₃₅Br,₃₇Rb and₃₉Y targets caused by protons over 300–400 keV energy range in 20 keV increment. The K-shell ionization cross sections (σ _k ^l ) at different energies were deduced from the K_α and K_β X-ray production cross sections which were obtained from X-ray yields of the K_α and K_β transitions. The experimental values are compared with the calculated values of ECPSSR theory and empirical reference cross sections. The resultant K-shell ionization cross sections are found to be in reasonable agreement with the ECPSSR theory. The K_α/K_β intensity ratios are also presented and compared with other experimental values and also with the theoretical one-hole values given by Scofield.     

Nb,Ag原子的K壳层和L壳层电离截面的理论计算

电子离子碰撞电离截面是模拟激光等离子体的超热电子的能谱和产额的主要过程之一.基于相对论性的电子离子碰撞的K壳层电离截面理论,计算了Nb、Ag的K壳层和L壳层电子碰撞电离截面,结果和最近的文献实验数值和其它理论数值进行了比较,计算结果比其它模型更加准确,与最近的实验结果也吻合较好,该结果可用来模拟激光等离子体的超热电子能谱和产额.     

电子碰撞引起的铜元素K壳层电离截面的测量与修正

 在电子碰撞的情形下,通过对铜靶的特征X射线测量,从而推算出它的K壳层电离截面。在实验中采用了薄靶厚衬底新方法。通过电子输运计算,由厚衬底产生的反射电子对计数的影响得以修正。用蒙特卡罗技术对质量厚度为23 mg∕cm²的铜靶的多次散射影响作了修正。     

Cross sections for K-shell ionization of Si and Ar by 4 keV to 10 keV electron impact

K-Auger electron emission of Si and Ar produced by 4 keV to 10 keV electrons was measured. Absolute yields were obtained by normalizing to the elastically scattered primary electrons. From the yields cross sections for K-shell ionization were deduced. The cross sections are in good agreement with the results of a fit formula for K-shell excitation in the whole range measured, while they agree with results of PWBA calculations including electron exchange in the Ochkur approximation only for the higher impact energies.     

Electronic relativistic effect on the ratios of deuteron to alpha-particle induced K-shell ionization cross sections

The ratios of the K-shell ionization cross sections induced by deuterons to those induced by α-particles with the same velocities have been calculated in the plane wave Born approximation using relativistic hydrogenic wave functions for the target electrons. The numerical results are compared with the recent experimental valus of Chang et al. The use of relativistic wave functios considerably improves the agreement with the experimental data.