Raman光谱法与经典方法验证阿司匹林固体分散体

为了验证Raman光谱法验证固体分散体的可行性, 采用熔融法制备阿司匹林固体分散体, 并用Raman光谱法和经典方法(红外光谱法和X-射线衍射法)研究其分散性。三种鉴别方法得到一致的结果--阿司匹林以微晶状态分散在固体分散体中, 且拉曼光谱法简单易行、快速直接、对样品无损伤, 是一种新的理想的检查固体分散体分散性的方法。     

半导体异质外延薄膜质量的X射线衍射检测方法

本文介绍了一种使用X射线宽角测角仪和双晶测角仪相配合的检测半导体异质外延薄膜的方法.其特点是快速且不损伤样品,特别适合大失配度的外延生长的条件试验检测,也可用于器件生产过程中的外延质量的监控.此法还可用于各种超晶格结构参数的测量.     

直接解调方法在嫦娥一号卫星X射线谱仪地面验证实验数据分析中的应用

"嫦娥一号"卫星是我国的第一颗月球探测卫星,运行轨道高度为200 km,预计工作寿命为一年,其上配备的X射线成像谱仪具备了对月表进行X射线探测、成像和对太阳X射线进行监测的功能.该X射线谱仪由两个全同的探测器阵列组成,其中,为了实现对月表主要化学元素分布及其含量进行探测的科学目标,在每个探测器阵列还配备了2个低能探测器单元.这4路低能探测器单元的面积为25 mm2,采用的都是厚度为500 μm,具有优良探测性能的Si-PIN探测器,其探测能区为1～10 keV,能量分辨率为～5%@5.9 kev.文章主要介绍了嫦娥一号卫星X射线谱仪的地面验证实验,并且根据X射线谱仪的能量响应矩阵,利用直接解调方法和基本参数法对X射线谱仪地面验证实验中的探测数据,特别是对盲测样品中的Mg,Al,Si等元素进行了定性和定量分析.     

考虑材料熔化潜热的高温高压本构

本文在修正的SCG模型基础上,提出了一种考虑了熔化潜热的高温高压本构.该本构所给出的铝的剪切模量的变化分为三个阶段：加工硬化,温度软化和熔化,并在完全熔化点处变为零.并且在前两个阶段,计算的结果与修正的SCG模型所给出的剪切模量的差别不超过4%,这一差别是在动高压实验误差范围之内的,在熔化区所给出的剪切模量与现有的实验数据相符合.关键词：剪切模量熔化潜热修正的SCG模型动高压实验     

高压屈服强度测量方法比较研究

对Asay-Chhabildas（AC）方法、横向应力计方法、压-剪方法和X射线衍射方法等4种高压动态屈服强度测量方法进行了比较,根据应变率的异同,将强度数据分为两类进行比较：X射线衍射方法和压-剪方法获得的强度与AC方法获得的强度Y=2c进行比较,而横向应力计方法测得的屈服强度与AC方法中的Y=2H进行比较。通过铝及其合金屈服强度数据的比较分析表明,AC方法、X射线衍射法和压-剪方法测得的强度数据基本一致,但横向应力计法测得的强度远高于AC方法测得的结果（Y=2H）,甚至高于其它3种方法测得的结果（Y=2c）。造成横向应力计方法测量结果异常的原因有待进一步研究。与实验数据的比较表明,Steinberg-Cochran-Guinan（SCG）模型过于依赖初始屈服强度,从而导致无法完全反映高压下材料的强度特性,模型有待进一步改进。     

高温高压下材料的本构模型

 在SCG模型基础上对其温度软化效应项作了改进,所提出的新模型在熔点温度T_m处满足剪切模量G(T_m)=0,从而提高了温度的适用范围。对Al和93W作了计算,其理论结果与实验符合相当好。     

Study of microstructure and nanomechanical properties of Zr films prepared by pulsed magnetron sputtering

The present work studies the effect of substrate temperature on the growth characteristics of zirconium films prepared by pulsed magnetron sputtering. Formation of α-phase of zirconium was observed in the temperature range 300-873 K. X-ray diffraction of Zr films revealed predominantly [0 0 1] texture. It is noticed that crystallite size increases with increasing substrate temperature. Hexagonal shaped crystallites seem to grow along the surface normal of the substrate for the films deposited at 773 K. Nanoindentation measurements showed that the hardness of the films is in the range 6-10 GPa. The scratch test indicated that the films deposited at higher substrate temperatures had excellent bonding with the substrate and no significant critical failure was noticed up to an applied load of 20 N.     

无氧铜动态卸载行为的数值模拟

分别利用Johnson-Cook（JC）本构模型和Steinberg-Cochran-Guinan（SCG）本构模型对无氧铜在10~20 GPa冲击压力下的卸载过程进行了数值模拟,与冲击-卸载实验结果比较表明,在这样的冲击压力下无氧铜的应变率效应仍然明显,JC模型对无氧铜的动态卸载行为有较好的描述。     

闪光照相中侧向散射的数值模拟

散射是闪光照相诊断技术中需要重点考虑的一个关键性问题,弄清散射的影响因素及其来源对于提高客体信息诊断精度具有十分重要的促进作用。针对法国实验客体照相系统,采用蒙特卡罗方法,系统研究了侧向散射的影响因素及其来源。结果表明:在没有侧向保护器的情况下,前保护器是侧向散射的主要来源,对任一点,前保护器的散射贡献均达到50%以上,并且侧向散射沿光轴方向呈递增或递减分布。在有侧向保护器情况下,侧向散射照射量有所减小,在与光轴垂直方向呈中间高两边低的单峰分布。增大侧向记录距离不一定带来侧向散射的降低。在适当的记录距离下,得到了较为均匀的散射分布。     

Protein immobilization capacity and covalent binding coverage of pulsed plasma polymer surfaces

Three carbon surfaces were deposited using pulsed plasma enhanced chemical vapour deposition method: a low and a high nitrogen-containing plasma polymer surfaces and a diamond-like carbon surface. The surfaces were analysed using both X-ray photoelectron spectroscopy (XPS) technique and the enzyme-linked immunosorbent assay (ELISA) method combining with sodium dodecyl sulphate (SDS) cleaning to investigate the capacity and covalent binding of the immobilized proteins. A good correlation was found on quantification of remaining protein after SDS cleaning using the ELISA method and the XPS technique. All surfaces had similar initial capacity of protein attachment but with large different resistance to SDS cleaning. The analysis showed that the high nitrogen-containing plasma polymer was the best biocompatible material due to its highest resistance to SDS cleaning, i.e. with the highest quantity (∼80%) of proteins bound covalently.     

载体MCM-41对Tb(aspirin)3phen发光性能的影响

在室温下,乙二胺环境中合成了高度有序的介孔材料MCM-41,并将经热处理的发光客体Tb(aspi-rin)3phen组装进其孔道,通过激发发射光谱对其光致发光性能进行了研究。结果表明,Tb(aspirin)3phen240～375 nm区间的宽激发峰归属于配体aspirin羰基n→π*跃迁、苯环π→π*跃迁,和phen的杂菲基团吸收,Tb3 的特征发射是由于Antenna效应引起的。相对于纯Tb(aspirin)3phen,Tb(aspirin)3phen-MCM-41B和Tb(aspirin)3phen/MCM-41A的激发谱带出现了明显的分裂,而Tb(aspirin)3phen-MCM-41A只在353nm处剩下了相对较窄的单峰。Tb(aspirin)3phen-MCM-41B,Tb(aspirin)3phen/MCM-41A和Tb(aspirin)3phen-MCM-41A的短波段激发峰依次减弱消失,长波段激发峰逐渐增强,而405 nm发射峰强度IL和544 nm发射峰强度ILn的比值I(I=IL/ILn)依次减小。MCM-41骨架与Tb(aspirin)3phen成键后,不同程度降低了配体aspirin和phen单重态S1和三重态T1能级,且对phen的影响大于aspirin。不同的MCM-41表面晶格场对配体能级的影响顺序为:MCM-41B外表面>MCM-41A外表面>MCM-41A内表面。I值可定性表示MCM-41表面晶格场对配体能级影响程度和MCM-41表面Tb(aspirin)3phen的含量。     

高能闪光照相中的能谱优化

在高能闪光照相技术中,提高图像接收平面上直穿与散射的比值有利于有效信息的提取。利用蒙特卡罗方法对法国实验客体的照相过程进行模拟,得到图像接收区域直穿分量与散射分量的能谱分布,依据其分布的特点提出了利用能谱优化来提高接收区域直散比的方法,指出添加衰减屏可以达到能谱优化的效果。依据线吸收系数的变化趋势以及实际加工的难度选择钽作为优化能谱的材料,并根据最小照射量的限制得到了最大的衰减屏厚度。最后通过蒙特卡罗模拟,指出添加9 mm的衰减屏能够对照相结果的优化程度最好,照射量满足要求,而直散比上升到原来的3倍左右。     

高能X射线辐射成像的定量模拟与密度重建

利用蒙特卡罗方法得到的数值图像研究高能X射线辐射成像的密度重建,提出多能X射线源、多材料客体辐射成像的密度重建方法.这种方法不仅能够对包括光源能谱、角分布和尺寸在内的密度重建,而且具有显含质量吸收系数的优点.利用约束共轭梯度算法和变分正则化技术进行法国试验客体的密度重建.结果表明,该方法能够有效地进行高能X射线辐射成像的密度重建,成像光子的能谱效应对于精确的密度重建十分重要.     

X光分幅相机-平面镜配接方法研究

利用X光谱仪用平面镜备件以及实验室常用五维调节架,设计了X光平面镜与X光分幅相机配接的探索方案,并对系统调节中各元件调节误差带来的影响进行了一定的分析,详细描述了系统的瞄准调节方法和过程.利用激光打靶实验,对X光平面镜与X光分幅相机的配接方法进行了检验.实验过程和结果表明,该方法系统结构和实施都较为简单,可以比较容易地在分幅相机微带上获得经平面镜反射的靶目标针孔像,实现～50ps的时间分辨、10～20μm的空间分辨及几十倍的能量分辨.     

X射线粉晶衍射仪的今天和明天

超能探测器(X’Celerator)的研制成功给X射线衍射仪的制造技术带来了革命性发展，录谱速度提高了100倍．而预校准光路模块化技术，使得各种测试功能可以在数分钟内准确地更换，无须重新调整光路，从而使长期以来一机多功能的期望得以实现．各种新型光学模块使得X射线衍射仪的利用率成倍提高，可以在短时间内获得高质量的衍射数据．新软件的推出，可以快速、准确、全面地给出相关衍射数据．     

X光透镜及其应用

着重介绍了Ｘ光透镜的原理,制作方法,及其在Ｘ光产业中的应用和发展前景。     

5—25keV刻度用X射线发生器

利用轫致辐射激发原子产生X射线荧光,经吸收边过滤,研制成单色低中能X射线发生器。实验给出5—25keV能区的4个单能点的强度、纯度以及相应的剂量率,可供刻度使用。     

嫦娥三号粒子激发X射线谱仪能谱温度影响的修正方法

粒子激发X射线谱仪(APXS)是中国探月工程二期嫦娥三号月球巡视器的有效载荷之一。简要介绍APXS的工作原理、组成部分,以及它在月面的工作环境,通过模拟及实验研究了月面热环境对APXS的影响,结果显示,APXS将工作在显著的变温过程中。相对恒温过程,APXS在变温过程中的能量分辨率明显变差。为了消除该温度效应的影响,提出了一种基于皮尔逊卡方检验(Pearson’s chi-squared test)的修正方法,能够有效提高变温过程中的能量分辨率。通过温度循环试验中变温阶段的数据对该方法进行了测试,结果表明,该方法具有很好的修正效果和较高的可靠性。     

Synthesis,growth and characterization of l-threonine zinc acetate (LTZA) NLO single crystal

Single crystals of l-threonine zinc acetate (LTZA) were grown from an aqueous solution by slow evaporation technique. Single crystal X-ray diffraction analysis reveals that the crystal belongs to monoclinic system. The optical transmission study reveals the transparency of the crystal in the entire visible region and the cut off wavelength has been found to be 350 nm. The optical band gap is found to be 3.55 eV. The microhardness studies reveal the mechanical strength of the grown crystal. The dielectric constant and dielectric loss were carried out for the grown crystal. Photoconductivity measurements carried out on the grown crystal reveal the negative photoconducting nature.     

Spectral spin diffusion and magnetic dipolar energy in the NMR of 13CH3 compounds

Spin diffusion between ¹³CH₃ groups in solids is studied both theoretically and experimentally. It is shown to be dominated by mutual spin flip–flops of protons belonging to neighbouring methyl groups. Also nonmethyl protons may contribute significantly if present in the sample. The spin–rotational ground state of ¹³CH₃ consists of 16 sublevels. When their populations are used to describe spin diffusion, eight population combinations are shown to be important, two of them corresponding to the ¹³C–proton and proton–proton intra-methyl magnetic dipolar energies, D_c and D_p, respectively. Spin-diffusion transitions modulate these combinations so that a further reduction to two sets of four combinations is possible, with no coupling between the sets. Coupled differential equations are derived to describe the time dependence of the combinations in each set. They are solved numerically and compared with experimental results on a single crystal of aspirin with ¹³C-labelled methyl groups at the carbon resonance. The ¹³C NMR induction signal was observed as a function of time after the preparation either at the carbon resonance (a two-pulse sequence) or at the proton resonance (proton saturation). Usually carbon spectra were computed first and then three of the mentioned population combinations were obtained from the individual spectral components. Some results on the time dependence of D_c were also obtained directly from the amplitude of the out-of-phase induction signal. Theoretical predictions are found to describe semiquantitatively the overall time dependence of these three combinations and especially their variation with different initial conditions, which are discussed in detail. Also the partial transfer of the magnetic dipolar energy between D_c and D_p is nicely explained. Reasons for discrepancies are discussed.