双重Q62重标度模型的重标度参数经验公式

结出了双重Q^2重标度模型的重标度参数经验公式,其中建立了重标度参数ξV,ξS及ξG与原子核平均结合能之间的联系,利用这套公式可以给出A≥12的所有核的重标度参数值,进而可以采用这些重标度参数值计算有关核过程做出预言。     

迈克尔逊风场干涉仪基准光程差及步长误差容限分析

迈克尔逊干涉仪风场探测是在一定的基准光程差的基础上,通过动镜步进或四分区镀膜的方法,获得一个波长范围内步进间隔为λ/4的四步干涉强度.在此过程中存在的基准光程差误差及步长误差将对结果产生影响.对在一定的结果不确定度允许范围内的误差变量的容限值进行了讨论.在可以预知的误差存在情况下的精确结果的得出给出了计算方法.     

二苯基亚砜、苯甲酸与轻稀土高氯酸四元配合物的合成表征及光致发光

合成并表征了高氯酸稀土与二苯基亚砜、苯甲酸的四种四元配合物。经元素分析、稀土络合滴定、摩尔电导率及差热-热重分析,表明四元配合物组成为[REL5L′(ClO4)] (ClO4) (RE= La,Pr,Nd,Eu;L=C6H5SOC6H5,L′=C6H5COO-)。在红外光谱中,第一配体二苯基亚砜的νS O的特征吸收峰出现在1 037cm-1处,而各稀土配合物的νS O向低波数移动到984 ～989 cm-1,红移50 cm-1左右,表明稀土离子与亚砜基团的氧原子之间发生配位作用。第二配体苯甲酸钠的反对称伸缩振动吸收峰νas(COO -)出现在1 550 cm-1,对称伸缩振动吸收峰νs(COO -)出现在1 416 cm-1处,羧基伸缩振动吸收频率差Δn[νas(COO -)-νs(COO -)]值为134cm-1;在所有配合物的红外光谱图中νas(COO -)向高波数方向发生了位移,而νs(COO -)向低波数方向发生了位移,并且Δn值均大于钠盐的Δn值,由此可以认为配合物中羧基是通过单齿方式与稀土离子配位。测定了配合物在丙酮溶液中的摩尔电导率,根据配合物在常见有机溶剂中的摩尔电导率与正负离子的关系结合配合物的红外光谱中高氯酸根离子的四条特征吸收带,表明配合物为1:1型电解质,两个ClO4-无机抗衡阴离子,其中一个在外界,一个进入内界与稀土离子配位。配合物的荧光发射光谱表明,四元配合物的荧光强度比二苯基亚砜高氯酸稀土二元配合物的荧光强度提高469%。磷光光谱表明苯甲酸三重态能级的下限和二苯亚砜三重态能级的上限重叠,导致三重态能级范围扩大,由此可见第二配体的加入提高了配体的三重态能级与Eu3 离子5D0能级的匹配程度。同时在配合物的荧光发射光谱中还可以看到铕离子的电偶极跃迁强度大于磁偶极跃迁,表明稀土离子不处于晶体场的对称中心。在四元配合物中,由于第二配体的加入,往往会降低配合物的对称性,从而增强稀土离子的荧光强度。本文合成的稀土配合物具有良好的荧光性能,而且在室温下稳定,溶解性好,分解温度较高。     

自引力场中非定态二维流体力学方程组的数值解

本艾以林家翘的线性密度波为初值,在自封闭边界的条件下,求得了自引力场中的非定态二维流体力学方程组的数值解.初始为基态5%的扰动密度,在10年的时间内会发展到与基态同量级.这表明,至少在气体盘模拟盘状星系时,星系密度波理论的准稳螺旋结构假设(Qsss 假设)需要作更进一步的考虑.     

Optimization of Metamorphic InGaAs Quantum Wells on GaAs Grown by Molecular Beam Epitaxy

We investigate the molecular beam epitaxy growth of metamorphic InxGal-xAs materials （x up to 0.5） on GaAs substrates systematically. Optimization of structure design and growth parameters is aimed at obtaining smooth surface and high optical qualdty. The optimized structures have an average surface roughness of 0.9-1.8 nm. It is also proven by PL measurements that the optical properties of high indium content （55%） InGaAs quantum wells are improved apparently by defect reduction technique and by introducing Sb as a surfactant. These provide us new ways for growing device quality metamorphic structures on GaAs substrates with long-wavelength emissions.     

Pb-Mg-Al合金腐蚀机理的电子理论研究

为了了解Pb-Mg-Al合金腐蚀的物理本质, 本文采用基于第一性原理的赝势平面波方法系统地计算了Pb-Mg-Al合金中各物相的结合能、费米能级和局域态密度等电子结构参数, 分析了合金的电化学腐蚀机理. 计算结果表明：Pb-Mg-Al合金中各主要组成物相稳定性大小关系为 Mg₁₇Al₁₂>Mg₂Pb>Mg;Mg,Mg₂Pb和Mg₁₇Al₁₂的费米能级存在E_f(Mg)>E_f(Mg₂Pb)>E_f(Mg₁₇Al₁₂)的关系, 说明Mg最容易失去电子, Mg₂Pb次之, Mg₁₇Al₁₂最难;局域态密度表明, 在同样的外界条件下, 体系中Mg相和Mg₂Pb相对于Mg₁₇Al₁₂均处于不稳定的状态, 容易失去电子, 即容易发生腐蚀. Pb-Mg-Al合金体系中不同物相的费米能级差构成了电化学腐蚀的电动势, 导致电子从费米能级高的Mg相和Mg₂Pb相流向费米能级低的Mg₁₇Al₁₂相, 使Pb-Mg-Al合金发生腐蚀.     

高压下Li掺杂p型ZnO固溶体的表征

报道了利用ZnO和Li₂O混合物在5GPa, 1200 ℃—1500 ℃条件下, 制备Li掺杂p型ZnO(记作ZnO: Li)固溶体的过程. 研究发现, 高压下温度对于ZnO: Li固溶体的导电类型以及结构具有较大的影响. 其中在1500 ℃条件下烧结的ZnO: Li(Li的掺杂量4.5%)表现出良好的p型电学性能, 其电阻率为3.1× 10^-1Ω·cm, 载流子浓度为3.3× 10¹⁹cm^-3, 迁移率为27.7cm²·V^-1·s^-1. 通过实验及理论计算确定了其受主能级为110meV, 讨论了压力对p型ZnO的形成和电学性能的影响.     

Temperature Controlled Filamentation in Argon Gas

Temperature controlled filamentation is experimentally demonstrated in a temperature gradient gas-filled tube. The proper position of the tube is heated by a furnace and two ends of the tube are cooled by air. The experimental results show that multiple filaments are shrunken into a single filament or no filament only by increasing the temperature at the beginning of the filament. This technique offers another degree of freedom of controlling the filamentation and opens a new way for intense monocycle pulse generation through gradient temperature in a noble gas.     

冰的熔解热实验中冰水质量比的探讨

冰与温水质量比对冰的熔解热实验的成败起着关键作用。文章对冰水质量比进行测量和分析,得出了冰的熔解热实验中最适合的冰水质量比的范围约为1／12-1／5。     

Complete low-frequency bandgap in a two-dimensional phononic crystal with spindle-shaped inclusions

A two-dimensional phononic crystal(PC) structure possessing a relatively low frequency range of complete bandgap is presented. The structure is composed of periodic spindle-shaped plumbum inclusions in a rubber matrix which forms a square lattice. The dispersion relation, transmission spectrum and displacement field are studied using the finite element method in conjunction with the Bloch theorem. Numerical results show that the present PC structure can achieve a large complete bandgap in a relatively low frequency range compared with two inclusions of different materials, which is useful in low-frequency noise and vibration control and can be designed as a low frequency acoustic filter and waveguides. Moreover,the transmission spectrum and effective mass are evaluated to validate the obtained band structure. It is interesting to see that within the band gap the effective mass becomes negative, resulting in an imaginary wave speed and wave exponential attenuation. Finally, sensitivity analysis of the effect of geometrical parameters of the presented PC structure on the lowest bandgap is performed to investigate the variations of the bandgap width and frequency.