新型大尺寸透中红外氧氟化物光学玻璃研究

红外光学玻璃是很多重要军、民用系统的关键窗口材料之一,但其高性能化、大尺寸化制备面临重要挑战。针对氟化物玻璃易挥发、抗析晶性能较差等特点,通过向含TeO2的氟铝酸盐玻璃中引入碱土金属氧化物BaO,显著降低了玻璃在熔制中的挥发,同时提高了玻璃的热稳定性。通过Raman光谱的分析,发现BaO的增加抑制了富TeO2玻璃分相,有利于碲酸盐玻璃与氟铝酸盐玻璃之间的融合,促进了玻璃网络结构的稳定。所得的氧氟化物红外光学玻璃有优异的红外透射性能,和氟化钙晶体性能对比,显示出低成本优势和更强的环境适应性。     

两个安全第一思想模型的比较分析

针对投资者可能的投资需求确立了基于安全第一思想下两个相近的投资目标:1、极大化投资末期总收益率超过给定水平α的概率;2、极小化投资末期总收益率与给定水平α的距离.并分别就这两个目标建立了优化决策模型,得到了模型解析解,最后对两个模型结果进行了比较分析和经济解释.     

Quantum State Transfer between Two Distant Atoms by Connecting Two Cavities via Optical Fibres

A scheme is proposed to unconditionally implement state transfer between two distant atoms by sending the atoms across two distant cavities connected via an optical fibre, respectively. The field state, which preserves the information about the first atom, is transmitted from one cavity to the other along the fibre. A Faraday rotator integrated in the fibre can be designed to completely stop the fields reflected from the second cavity, thus after the field interacts with the second atom for a defined time, the state transfer can be accomplished with unit efficiency.     

沸石催化剂上醇的醚化反应

研究了乙醇，正丁醇，仲丁醇和正戊醇有ＺＳＭ－５和Ｂｅｔａ沸石上的醚化反应。用ＮＨ３－ＴＰＤ和ＩＲ测定了ＺＳＭ－５沸石的表面酸性，讨论了沸石表面Ｂ酸和Ｌ酸和与醚化活性的关系。结果表明，乙醇的脱水反应既可以在Ｂ酸中心上进行，也可以在Ｌ酸中心中心上进行，既可以在强酸中心上进行，亦可以在弱酸中心上进行。     

ZrO2/SiO2溶胶-凝胶薄膜膜层间的渗透行为

分别以丙醇锆和正硅酸乙酯为原料,采用溶胶-凝胶工艺制备了性能稳定的ZrO2和SiO2溶胶。用旋转镀膜法在K9玻璃上分别制备了单层SiO2薄膜、单层ZrO2薄膜、ZrO2/ SiO2双层膜和SiO2/ZrO2双层膜。采用原子力显微镜观察了薄膜的表面形貌,用椭偏仪测量薄膜的厚度与折射率,用紫外-可见光分光光度计测量了薄膜的透射率。对薄膜的透射光谱和椭偏仪模拟的数据进行分析,发现SiO2/ZrO2双层膜之间的渗透十分明显,而ZrO2/SiO2双层膜之间几乎不发生渗透。利用TFCalc模系设计软件,采用三层膜模型对薄膜的透射率进行模拟,得出的透射曲线与用紫外-可见光分光光度计测量的透射曲线十分符合。     

Near threshold photodetachment cross section of negative atomic oxygen ions

A 40-target state close-coupling calculation for the photodetachment cross section of negative atomic oxygen near threshold is carried out with core－valence electron correlation by using the R-matrix method. It was shown that after considering the excitations of two electrons from the 2s shell, the electron affinity of O^- (2s^22p^5{}^2P°) agrees with the experimental result much better than that just considering the excitations of electrons only from the 2p shell as well as only one electron from the 2s shell. Total cross section as well as the main contribution of the ionization channels to the partial cross section are illustrated to show the structure near threshold clearly.     

利用点在圆锥曲线内(外)部解“范围”问题

利用点在圆锥曲线内（外）部解“范围”问题袁兴发（陕西镇巴县中学７２３６００）已知圆锥曲线Ｃ上存在不同的两点关于直线ｌ（含参数）对称，求参数的范围，对这类问题，这里介绍一种解法，即利用点在曲线内部或外部导出不等式，从而确定参数的取值范围．圆锥曲线的含焦...     

Spectra and Spin Polarization of the Valence Band Auger Emission from Cr （100） Surface

Calculations have been carried out on spin-polarized Auger electron emission from a seven-layer chromium (lO0)-film. The core and valence states concerning the Auger transition are obtained from a self-consistent full-potential linearized augmented plane wave calculation by using a repeated slab geometry. The calculations refer to experiments on the L3M23 V- and L3 VV-transRions that have recently been carried out by Heinzmann et al. The Auger spectrum obtained for the L3VV transition agrees relatively well with our calculations, whereas the observed L3M23V-Auger structure is considerably wider than that predicted by our theory. Nevertheless, the spin-polarization in the latter case, which is about -13%, is in fair agreement with the experiment, different from the L3VV-transition where the experiment yields -10% as opposed to the theoretical value of -25%. We give possible reasons for the origin of these discrepancies.     

Laminar boundary layer between two planes perpendicular to each other

In this paper, we obtain a third-order approximate solution for the laminar boundary layer between two planes perpendicular to each other.In boundary layer equations, the viscous and the inertial terms have the same quantity step. In this paper, at first, supposing that the inertial terms are bigger than the viscous terms, we solve the boundary layer equations, and then we suppose that the viscous terms are bigger than the inertial terms. At last, we take the mean value as the valid solution of the boundary layer equations.The first- and the second-order approximate solutions obtained in this paper coincide with the results in ref. [1], while the third-order solution obtained in this paper is better than that in ref. [1].