X射线（n,—n）双晶衍射抑制高次谐波实验研究

对将用于同步辐射ＥＸＡＦＳ 实验站双晶单色器的晶体进行了双晶衍射失谐抑制高次谐波的实验．结果表明，对Si(111）晶体，当双晶衍射失谐到基波强度只有原来的一半时，高次谐波均消失．本文讨论了Si（２２２）衍射不完全消光的原因．对Si（２２０）晶体衍射的情况也进行了简要的讨论．     

X射线双晶衍射摇摆曲线本征半峰宽的理论计算

本文应用X射线衍射动力学理论,推导出Bragg衍射几何X射线双晶衍射反射率的数学表达式。多种晶体、不同衍射的摇摆曲线计算结果表明,σ偏振的摇摆曲线的峰值和积分强度均比π偏振的高。而且半峰宽较宽。同时指出,对圆偏振X射线入射或者A,B两晶体不同类或者两者的衍射级数不相同时,很多文献给出的双晶衍射摇摆曲线半峰宽的近似表达式2^1/2∞不再适用。 关键词：     

薄膜物理及其应用讲座 第十讲 低维材料的X射线衍射(Ⅰ)

综合介绍了高分辨Ｘ射线双晶衍射技术、三轴晶衍射技术及掠入射衍射和全反射技术．着重介绍了这些技术应用于低维材料微结构探测所取得的新进展．     

MOCVD生长的GaN单晶膜透射光谱研究

采用MOCVD技术在Al2O3(0001)衬底上生长了GaN薄膜，使用透射光谱、光致发光光谱和X射线双晶衍射三种技术测试了五类GaN薄膜样品，实验结果表明：GaN薄膜透射谱反映出的GaN质量与X射线双晶衍射测量的结果一致，即透射率越大，半高宽越小，结晶质量越好；而X射线双晶衍射峰半高宽最小的样品，其PL谱的带边峰却很弱，这说明PL谱反映样品的光学性能与X射线双晶衍射获得的结晶质量不存在简单的对应关系，同时还报导了一种特殊工艺生长的高阻GaN样品的RBS／沟道结果。     

应变弛豫InGaAs/GaAs超晶格的X射线双晶衍射及形貌研究

应用X射线双晶衍射及双晶形貌术,对应变弛豫的InGaAs/GaAs超晶格作了研究,通过对双晶衍射摇摆曲线的计算机模拟,得到了超晶格的结构,应变弛豫机制,弛豫比,超晶格层与衬底的取向差等重要参数。从双晶形貌,得到了超晶格与衬底界面处和超晶格中的位错分布。 关键词：     

AlGaAs/GaAs波导薄膜X射线双晶衍射研究

本文应用X射线双晶衍射研究AlGaAs/GaAs波导结构薄膜。结合实验结果,应用X射线衍射动力学理论。计算衬底和多层膜的反射强度,得到样品的真实结构。分析影响薄膜双晶衍射摇摆曲线的若干因素。 关键词：     

MOCVD生长的未掺杂GaN的结晶特性与补偿度关系的研究

对本实验室用ＭＯＣＶＤ方法生长的未故意掺杂的ＧａＮ单晶膜进行了结晶性能、电学性能研究。结果表明,室温时ＧａＮ的Ｘ射线双晶衍射半高宽与其补偿度有较强的依赖关系。高补偿的ＧａＮ的Ｘ射线双晶衍射半高宽较宽。低补偿的ＧａＮ的Ｘ射线双晶衍射半高宽较窄。     

双晶单色器弧矢聚焦晶体面形有限元分析

简要介绍了弧矢聚焦双晶单色器的基本原理、聚焦晶体的压弯以及鞍形形变的抑制,提出了柔性铰链弧矢聚焦晶体压弯机构,对弧矢聚焦晶体衍射面的子午形变和弧矢弯曲面形进行了有限元分析;用光学追踪程序SHADOW得出了弧矢聚焦晶体衍射面面形对单色器的光通量和分辨率的影响。     

45°内反射镜高功率InGaAs/AlGaAs/GaAs面发射半导体激光器结构设计和制备

研究了具有45°内反射镜的0 98μm辐射波长的应变InGaAs/AlGaAs/GaAs单量子阱面发射半导体激光器结构,并采用MBE方法进行了材料制备。同时利用X射线双晶衍射,低温(10K)光致发光(PL)和电化学C V方法检测和分析了外延薄膜的光电和结构特性。在光致发光谱线中我们得到了发射波长0 919μm的谱峰,谱峰范围跨跃0 911～0 932μm,双晶回摆曲线、电化学C V分布曲线显示所设计的结构基本得到实现。     

发光多孔硅表面微结构及其晶格畸变的实验研究

用电化学方法制备了不发光多孔硅和发光多孔硅,用X射线双晶衍射对两类多孔硅表面进行了微结构分析和晶体质量表征,实验表明两类多孔硅的微结构间存在着很大差别。不发光多孔硅表面对X射线的双晶衍射摇摆曲线可解叠成两个峰,它们分别来自样品多孔层和单晶硅衬底,而发光多孔硅对X射线的双晶衍射摇摆曲线呈高斯对称分布,不可解叠。发光多孔硅比不发光多孔硅表面晶体质量差,且电化学腐蚀越严重,表面晶体质量下降也越严重。     

On Slant Magnetic Curves in S-manifolds

We consider slant normal magnetic curves in (2n + 1)-dimensional S-manifolds. We prove that γ is a slant normal magnetic curve in an S-manifold (M^2m+s, φ, ξ^α, η^α, g) if and only if it belongs to a list of slant φ-curves satisfying some special curvature equations. This list consists of some specific geodesics, slant circles, Legendre and slant helices of order 3. We construct slant normal magnetic curves in ?2^n+s(–3s) and give the parametric equations of these curves.     

平面约束下金属铁磁条中平行抽运微波磁场的非稳定阈值研究

运用Landau-Lifshitz方程，边界处动态磁化强度由有效偶极边界条件约束，研究了无限长金属磁条中自旋波传播的特征，得到了该体系抽运微波磁场的阈值曲线以及色散曲线的解析式，揭示出自旋波激发谱与磁条宽度的具体关系.结果表明，平面约束下磁条的阈值曲线中出现了明显的扭结现象.并且随着磁条宽度的增加，其扭结数近似地呈指数形式增加，而最低扭结处两阈值的跳跃差值几乎呈反比形式变化. 关键词： Landau-Lifshitz方程 有效偶极边界条件 阈值曲线 色散曲线     

ZFA等角距曲线的优化设计

变焦距系统镜组的轴向位移与倍率关系通常不是线性的,示值间距标记也是非均匀的。在光学检测和计量仪器的应用中,操作者很难准确地选择刻度标志之外的焦距值,尤其是在高倍段刻度密集的和非线性显著的地方更是如此。在有电机驱动的系统中,电机匀速转动带来的是倍率的非线性变化,很难在短时间内稳定到预定倍率的目标值。对含有像差因子的变焦函数进行变换后所编制的计算程序可以十分快捷地得到预定的设计结果。一个实际的光学系统往往偏离理想情况,为了达到最佳结果,可把像差因子补充到变焦距函数中,可借助变焦函数方程进行等角距变倍曲线的研究和设计,研究成果已应用到了产品的设计中,并取得了很好的效果。     

磁开关作为脉冲驱动源主开关的实验研究

使用矩形截面磁芯研制了一台磁开关作为脉冲驱动源的主开关,并利用电容器放电法对磁芯不同位置处的磁滞回线进行了测量。结果表明,短边和长边测量得到的磁滞回线均能够适应磁开关需求,不同的励磁位置对磁滞回线形状的影响有限。设计了基于该磁芯的磁开关,使用PSpice软件进行了数值模拟,结果与理论分析相一致。结合卷绕型带状脉冲形成线,对磁开关作为脉冲驱动源主开关进行了实验研究。结果表明研制的磁开关实现了主开关功能,在1.1 的低阻抗负载上获得了峰值电压9 V、上升沿80 ns、脉冲半高宽230 ns的准方波脉冲输出。     

闪光照相中源尺寸和散射对成像的影响

 利用Monte Carlo(MC)模拟技术解释实验中心线灰度曲线的各部分波形。结果发现，系统中的散射照射量、光源的尺寸和H-D特征曲线的形状对实验灰度曲线的各部分波形均有影响：散射量越大，中心信号幅度越低;H-D曲线趾部的非线性越严重，中心信号幅度也越低;光源尺寸造成图像越模糊。指出了用实验波形可以半定量确定系统散射程度和光源尺寸。在测量照射量时，应该尽可能避免散射的干扰,用台阶法测量H-D曲线时，应使台阶远离剂量片而前移。     

3D combinational curves for accuracy and performance analysis of positive biometrics identification

The receiver operating characteristic (ROC) curve has been widely used as an evaluation criterion to measure the accuracy of biometrics system. Unfortunately, such an ROC curve provides no indication of the optimum threshold and cost function. In this paper, two kinds of 3D combinational curves are proposed: the 3D combinational accuracy curve and the 3D combinational performance curve. The 3D combinational accuracy curve gives a balanced view of the relationships among FAR (false alarm rate), FRR (false rejection rate), threshold t, and Cost. Six 2D curves can be derived from the 3D combinational accuracy curve: the conventional 2D ROC curve, 2D curve of (FRR, t), 2D curve of (FAR, t), 2D curve of (FRR, Cost), 2D curve of (FAR, Cost), and 2D curve of (t, Cost). The 3D combinational performance curve can be derived from the 3D combinational accuracy curve which can give a balanced view among Security, Convenience, threshold t, and Cost. The advantages of using the proposed 3D combinational curves are demonstrated by iris recognition systems where the experimental results show that the proposed 3D combinational curves can provide more comprehensive information of the system accuracy and performance.     

Real-time adjustment of optical transmitter by laser beam parameter measurement based on two linear array CCD scanning imaging

In this paper, we present a real-time measurement and adjustment method, based on scanning imaging, for optical transmitter which emits 90° × 2° linear laser beam. This novel optical arrangement consists of an area array CCD and two linear array CCDs. According to the relationship between the positions, angles of transmitter optical components and the beam parameters of emergent laser, the system can help us to decide the real-time adjustment of optical transmitter by measuring the related beam parameters. In order to improve the measurement speed, avoid occlusion and ensure simultaneous measurement, the two linear array CCDs are placed at near field, far field and separated by a definite angle to acquire the beam intensity distribution through suitable nonlinear correction during the process of scanning. After a complete scanning, the beam parameters and the spot image are acquired by continuous measurement. The proof-of-principle experiments showed that the measurement results were in agreement with the analysis. The presented method was applied to direct fast adjustment for higher quality on the assembly of the optical transmitter. The presented procedure is highly advantageous for diverse laser beam emitted from the optical transmitter, such as elliptic, linear and so on.     

Null Cartan Bertrand curves of AW(k)-type in Minkowski 4-space

This Letter considers the curvature conditions of AW(k)-type (k=1,2,3)$(k=1,2,3)$ null Cartan curves, and investigates null Cartan Bertrand curves. We show that null Cartan Bertrand curves are AW(k)-type (k=1,2,3)$(k=1,2,3)$ curves in Minkowski 4-space.     

一个驻波演示实验

介绍一个驻波演示实验，让声波在充有可燃性气体的圆管中形成驻波，气体通过多孔燃烧时出现余弦分布的火焰包迹线，这个包迹线能把驻波显示出来。