AFS-230型双道原子荧光光度计的安装与验收

本文简述北京海光仪器公司生产的ＡＦＳ 2 30型双道原子荧光光度计安装条件的要求、安装过程应注意的问题以及如何调试验收指标。1　仪器安装1.1　拆箱检查包装箱有无变形和受损 ,取出仪器 ,检查外观有无损坏 ;对照装箱单检查各配套件及备件是否齐全。1.2　仪器使用环境条件室内工作温度 :15～ 35℃、湿度≤ 75 % ;仪器应远离强电磁场及冲击振动源 ;由于所测试的元素为有毒物质 ,为保证工作人员的安全 ,本仪器应配有强制排风系统。1.3　电源仪器供电电压为 (2 2 0± 2 2 )Ｖ、频率为 (5 0± 1)Ｈｚ的正弦交流电源 ,消耗功率 >10 0 0Ｗ ,电压…     

拟线性双曲方程组一类广义Riemann问题的整体间断解

对一阶拟线性双曲方程组一类广义Riemann问题，该文在一定条件下证明了，包含一个接触间断和一个中心波以及包含一个接触间断和一个激波的间断解的整体存在性和唯一性.     

一种高精度保界的守恒重映方法

Lagrange方法中，当流场发生大变形时，跟踪流体运动的Lagrange网格发生扭曲，使计算无法进行下去，此时必须重分网格，把网格修复成较好的形状。另外，网格自适应技术中的重构、合并与加密，以及同一问题不同程序相继计算的连接，并行计算中相邻块边界区域的数据传递等，这些情况都需要利用旧网格上的物理量来确定新网格上的物理量，是一个物理量重映过程。质点重映方法是基于物理上守恒规律的一种离散的物理量守恒映射方法，既可实现分片常数分布的一阶精度重映计算，又可实现分片线性分布的二阶精度重映计算。这种方法可严格保证守恒量的守恒性，且可以实现任意多边形网格以及节点上物理量的守恒重映。但是，基于分片线性分布的二阶精度重映方法，如果新网格的守恒量没有进行保界调整，那么相应的强度量有可能在其局部的限制范围之外，破坏了原网格物理量的单调性。因而，对二阶精度的质点重映方法进行了进一步研究。在分片线性分布的基础上，将基于结构网格的保界算法扩展到非结构网格上，给出了二阶保界的质点守恒重映方法。     

p型导电掺In的SnO_2薄膜的制备及表征

采用溶胶 凝胶提拉法成功地制备了p型导电掺In的SnO2 薄膜 .x射线衍射测试结果表明 ,掺In的SnO2 薄膜保持SnO2 的金红石结构 .吸收谱测试结果表明 ,掺In的SnO2 禁带宽度为 3 8eV .霍尔测量结果表明 ,空穴浓度与热处理温度有很大的关系 ,5 2 5℃为最佳热处理的温度 .铟锡原子比在 0 0 5— 0 2 0范围内 ,空穴的浓度与In的含量有直接的关系 ,并随In含量的增加而增加     

小型企业规模的有效性分析

在当代企业纷纷追求规模的不断扩大的同时，统计数据却显示企业平均规模不断下降的事实趋势。论根据数学、经济学与博弈论的有关理论对企业规模小型化的内在要求进行了探讨，分析的结论一致证明：粘型化规模在当代经济环境中是充分有效的。     

Lie symmetries and conserved quantities of controllable nonholonomic dynamical systems

This paper concentrates on studying the Lie symmetries and conserved quantities of controllable nonholonomic dynamical systems. Based on the infinitesimal transformation, we establish the Lie symmetric determining equations and restrictive equations and give three definitions of Lie symmetries before the structure equations and conserved quantities of the Lie symmetries are obtained. Then we make a study of the inverse problems. Finally, an example is presented for illustrating the results.     

Chiral Parameter of Transparent Films Containing Polymer Cholesteric Liquid Crystal-R

The transparent film containing a kind of polymer cholesteric liquid crystal-R was fabricated by the freezing method. The optical polarization response of the film was investigated by a self-manufactured apparatus and its optical rotatory dispersion was measured by a novel technique at the wavelength from 35Onto to 66Onto.At various wavelengths, the chiral parameter of the film has been obtained. The results show that the chiral parameter decreases as the wavelength increases. The maximum and minimum chiral parameters are 0.0343 at the wavelength of 350 nm and 0.0058 at the wavelength of 660 nm, respectively. The obtained data indicate that this kind of polymer cholesteric liquid crystal-R is a promising candidate host material for solid optical chiral waveguides.     

Proton Fraction in Neutron Star Matter and Three-Body Force Effects

The three-body force effects on the equation of state and its iso-spin dependence of asymmetric nuclear matter and on the proton fraction in neutron star matter have been investigated[1] within Brueckner Hartree-Fock (BHF) approach by using a microscopic three-body force. It is shown that, even in the presence of the three-body force, the empirical parabolic law of the energy per nucleon vs. isospin asymmetry β=(N-Z)/A is fulfilled in the whole asymmetry range 0 ≤β ≤1 and also up to high density. The three-body force provides a strong enhancement of symmetry energy at high density in agreement with relativistic approaches. Thecalculated proton fraction in β stable neutron star matter is given in Fig.l, where the thick solid line is the BHF prediction using AV18 TBF, while the dotted one is the BHF result using AVis. The thin solid line is the prediction of the Dirac-Brueckner approach taken from Ref.[2]. The results extracted according to the phenomenological paramete rizations of the symmetry energy suggested in Ref.[3] are also plotted. It is seen from     

关于高阶中立型偏微分方程系统解的振动性

近年来,由于偏泛函微分方程(组)理论在人口动力学,生物遗传工程和化学反应过程等领域中有广泛的应用,因而很多学者在偏泛函微分方程(组)解的振动性理论的研究方面做了大量工作,取得了许多成果.本文将研究一类较广泛的高阶中立型偏微分方程组     

利用拉曼型的Jaynes-Cummings模型传送两比特的未知原子态

实现量子态的隐形传送、尤其是多比特量子态的隐形传送在量子信息领域中有非常重要的作用，提出了一种隐形传送两比特未知原子态的方案，在此方案中，用两个两粒子纠缠态代替一个三粒子纠缠态作为量子信道，而且此方案可推广到隐形传送N比特的未知原子态。