利用光致聚合物的真彩色反射全息图

本文用Ar~+-Kr~+激光器的红光(647.1nm)、绿光(574.5nm)和蓝光(488.0nm)分别对准全色的光致聚合物干板制作反射光栅,给出各个反射光栅的光谱透射率曲线,由此可得最小透射率随曝光量、再现波长随曝光量变化的情况.并采用Ar~+-Kr~+激光器全谱线输出和减色滤光片一次曝光成功地拍摄了真彩色反射全息图.本文还讨论了彩色反射全息图再现像的色度坐标和彩色控制.     

均分散胶体的研究──Ⅷ．草酸钛酰钡均分散颗粒的制备、组成及应用

本文提出了制备草酸钛酰钡均分散颗粒的优选条件．对此条件下制备的均分散颗粒进行了化学分析、ＴＧＡ、ＩＲ分析并确定了其化学组成．将此种颗粒灼烧成氧化物后，基本上可保留原形貌．用ＢａＯ·ＴｉＯ２均分微颗粒与Ｙ２Ｏ３均分散颗粒烧制成ＢａＴｉＯ３均分散陶瓷，以达到控制陶瓷超微结构均匀的目的．     

弹核碎裂反应中同位旋效应的系统研究

用统计擦碎模型对中能区不同弹靶体系在弹核碎裂反应中的同位旋效应和同位旋标度率现象进行了系统研究. 发现归一的同位素分布峰位差和约化的同位旋标度率参数随(Z_proj－Z)/Z_proj or (N_proj－N)/N_proj呈指数下降, 与反应系统大小无关. 指出约化的同位旋标度率参数可以用来研究中能重离子碰撞中反应系统的激发程度和非对称核物质的状态方程.     

一道数学高考题的巧解及推广

例1　求ｃｏｓ270° ｃｏｓ250° ｃｏｓ70°·ｃｏｓ50°的值.按常规解法,这道题一般是先降次,再和差化积,积化和差.但过程较繁,现给出一种解法如下.解　设ｘ=ｃｏｓ270° ｃｏｓ250° ｃｏｓ70°·ｃｏｓ50°,ｙ=ｓｉｎ270° ｓｉｎ250° ｓｉｎ70°·ｓｉｎ50°,则ｘ ｙ=2 ｃｏｓ20°(1)　ｘ-ｙ=ｃｏｓ140° ｃｏｓ100° ｃｏｓ120°=2ｃｏｓ120°ｃｏｓ20°-12=-ｃｏｓ20°-12(2)(1) (2)得2ｘ=32,即ｘ=34.∴ｃｏｓ270° ｃｏｓ250° ｃｏｓ70°ｃｏｓ50°=34.现在,我们把这道题推及一般.例2　求ｃｏｓ2α ｃｏｓ2β ｃｏｓαｃｏｓβ在…     

均分散胶体的研究──Ⅷ.草酸钛酰钡均分散颗粒的制备、组成及应用

本文提出了制备草酸钛酰钡均分散颗粒的优选条件.对此条件下制备的均分散颗粒进行了化学分析、TGA、IR分析并确定了其化学组成.将此种颗粒灼烧成氧化物后,基本上可保留原形貌.用BaO·TiO₂均分微颗粒与Y2O₃均分散颗粒烧制成BaTiO₃均分散陶瓷,以达到控制陶瓷超微结构均匀的目的.     

Cross Sections of Elastic Electron and Positron Scattering from Proton-Rich Nuclei

We investigate the cross sections of the elastic electron or positron scat tering from 208 Pb, ^12C ^12,16O and ^28,32S by the relativistic partial-wave expansion method using the static charge density distribution from the self-consistent relativistic mean fiel model and also calculate the charge form factor for ^12＇16O and ^28,32S. The numerical results are compared with the available data. Calculations indicate that the extended charge density distributions of ^12O and ^28S have observable effects on the cross sections of the electron or positron scattering as well as the charge form factors.     

聚晶金刚石复合片热残余应力分布规律实验研究

利用改进的应力释放法、X射线衍射法以及Raman光谱,对平面界面结构金刚石复合片表面热残余应力分别进行了实验研究,得到了金刚石层表面热残余应力值及其分布规律,同时得到了基体厚度与热残余应力的相关关系.研究结果表明,采用应力释放法、X射线衍射法及Raman光谱法测试PDC表面热残余应力,其测试结果均与有限元分析结果相吻合,证明了这三种方法的有效性.其中,X射线衍射法测试结果的误差最大,应力释放法其次,Raman光谱法最为精确.由于应力释放法应变片尺寸及X射线衍射法光斑照射范围的限制,无法在试样表面上取较多的测试点,因此难以得到理想的热残余应力分布曲线.而Raman光谱法中所采用的激光光斑仅5μm,可以取更多的测试点,因此其结果更能真实的反映金刚石层表面热残余应力的分布规律.本文的研究结果为精确测试PDC热残余应力,从而为优化PDC界面结构、提高PDC使用性能提供了理论和实验依据.     

Scaling of anisotropic flows and nuclear equation of state in intermediate energy heavy ion collisions

Elliptic flow ($v_2$) and hexadecupole flow ($v_4$) of light clusters have been studied in detail for 25 MeV/nucleon $^{86}$Kr + $^{124}$Sn at large impact parameters by using a quantum molecular dynamics model with different potential parameters. Four sets of parameters including soft or hard equation of state (EOS) with or without symmetry energy term are used. Both number-of-nucleon ($A$) scaling of the elliptic flow versus transverse momentum ($p_{\rm t}$) and the scaling of $v_4/A^{2}$ versus $(p_{\rm t}/A)^2$ have been demonstrated for the light clusters in all above calculation conditions. It is also found that the ratio of $v_4/{v_2}^2$ maintains a constant of 1/2 which is independent of $p_{\rm t}$ for all the light fragments. Comparisons among different combinations of the EOS and the symmetry potential term show that the above scaling behaviours are sound and independent of the details of potential, while the strengths of flows are sensitive to the EOS and the symmetry potential term.     

Ni-Co-B非晶态合金催化肉桂醛常压加氢制3-苯丙醛的研究

采用化学还原法制备了一系列Ni-Co-B非晶态合金催化剂, 通过调变金属盐混和液中Ni^2＋/Co^2＋的比例, 可制得不同Co含量的Ni-Co-B非晶态合金. 用ICP, BET, XRD, TEM, SAED, DSC, XPS和H₂-TPD对其组成、结构、粒子大小、表面形貌和表面电子态进行了系列表征, 并以肉桂醛常压加氢制苯丙醛作为探针反应, 考察了所制备的Ni-Co-B非晶态合金的催化性能. 结果表明, Ni-Co-B非晶态合金中Ni为活性中心, Co的引入可显著增加其催化活性. 由于催化测试中金属总量固定为1.0 g, 因此增加Ni-Co-B中Co的含量具有正负两方面的效应. 一方面, 由于Ni活性位数目的减少加氢活性降低; 另一方面, Co对Ni活性中心具有协同作用, 有利于增加合金的无序度、金属-类金属间相互作用、表面Ni含量和电子相互作用, 从而提高催化活性. 最佳Co与(Ni＋Co)摩尔比含量的范围为0.2～0.5.     

Isoscaling of projectile-like fragments

In this paper, the isotopic and isotonic distributions of projectile fragmentation products have been simulated by a modified statistical abrasion--ablation model and the isoscaling behaviour of projectile-like fragments has been discussed. The isoscaling parameters α and β have been extracted respectively, for hot fragments before evaporation and cold fragments after evaporation. It looks that the evaporation has stronger effect on α than β. For cold fragments, a monotonic increase of α and β with the increase of Z and N is observed. The relation between isoscaling parameter and the change of isospin content is discussed.