Calculation of α decay half-lives for superheavy elements using the double folding model＊

α decay half-lives of some new synthesized superheavy elements, possibly synthesized superheavy elements and decay products are calculated theoretically within the WKB approximation by using microscopic α-nucleus interaction potentials. These nuclear potentials between the α particle and daughter nuclei are obtained by using the double folding integral of the matter density distribution of the α particle and daughter nuclei with a density-dependent effective nucleon-nucleon interaction, in which the zero-range exchange term is supplemented. The calculated α decay half-lives are compared with those of the different models and experimental data. It is shown that the present calculation successfully provides the half-lives of the observed decays for some new superheavy elements and therefore gives reliable predictions for α decay of possibly synthesized superheavy elements in future experiments.     

Synthesis, Characterization, Crystal Structure and Stability of a Ternary Cu(Ⅱ) complex with 1,10-Phenanthroline and L-Valinate

Introduction It is important to research the mixed-ligand copper complexes containing bioligands,such as amino acids, nucleic acids and proteins,in exploring the functional mechanism of microelement copper in organism because the reaction of any micronutrient with two or more bioligands in the concentrated bioligands background gives mixed-ligand ternary complexes, which are more stable[1]and related with storage of substance and transportation of metal ions in the life process.     

GC-MS分析氧化亚铁硫杆菌培养液的挥发性成分

GC- MS联用技术对耐强辐射微生物氧化亚铁硫杆菌 [Thiobacillus ferroxidans(T.f) ]的挥发性代谢产物进行了研究 ,发现 4 3种代谢物 ,由标准谱图鉴定了其中 2 3种化合物。     

DAIP改性环氧树脂研究

采用共固化的方法,得到酚醛环氧树脂(F-51)和间苯二甲酸二烯丙基酯(DAIP)的共固化树脂。实验结果表明:DAIP的加入降低了F-51环氧树脂的粘度[体系粘度为150～350mPa·s(25℃)],利于工艺操作;提高了F-51环氧树脂的耐热性,热变形温度达200℃。研究了F-51环氧树脂和DAIP共固化的固化行为、不同配比对共固化物形态结构的影响;并研究了不同配比对固化物耐热性的影响。     

氯醇盐溶胶-凝胶法纳米结构氧化钨薄膜的光谱学特性

由非离子型Gemini表面活性剂TMDD(HO(EO)xC14(EO)yOH)为结构导向模板, 改进EISA(挥发诱导自组装)镀膜工艺经300 ℃焙烧制得具有连续、均一和光学透明特点的蠕虫介孔纳米晶孔壁氧化钨薄膜. 采用SEM、TEM和Raman光谱对此种薄膜的介孔纳米结构进行了表征, 通过光谱电化学、XPS和椭偏谱等方法, 研究了该薄膜在电解质溶液中的电致变色行为. 结果表明, 所制备的纳米结构氧化钨薄膜在633 nm波长处的循环可逆透过率调制幅度可达75%以上, 并且其电致变色机理具有显著的双注入吸收调制特性.     

Lattice Boltzmann模型在CFD中应用

近年来,格子Boltzmann方法(LBM)已发展为一种模拟流体和物理问题的新颖的、有前景的数值方法,在许多领域的各种数值问题求解上取得很大的成功.文章介绍了一种模拟复杂流动的高效建模数值算法Lattice Boltzmann方法,和它的基本原理及其应用.并通过两个实例数值模拟计算,说明Lattice Boltzmann方法正确、有效,并展示了广阔的应用前景,为今后更深入的研究和广泛应用打下基础.     

On the Diophantine Equation x2 - kxy ＋ y2 ＋ 1x = 0

Let l be a given nonzero integer.The authors give an explicit characterization of the positive integer k that makes the Diophantine equation x2-kxy+y2+lx=0 have infinitely many positive integer solutions(x,y).     

FTIR光谱仪中基于定镜调整的动镜运动控制研究

动镜是FTIR光谱仪中唯一不断运动的部件,动镜的匀速运动性能以及动镜与定镜的准直性好坏影响干涉效果和光谱图质量,直接制约着仪器的精度和分辨率,对仪器整体指标起着重要作用。文章围绕FTIR光谱仪中干涉仪动镜运动的匀速性以及其与定镜的准直性展开研究,使用相位检测技术对定镜的姿态作出动态调整以补偿动镜与定镜间的倾斜夹角,并且设计了具有磁悬浮特点的动镜支撑系统。文章采用改进的模糊PID控制算法实现动镜运动速度的精确调节,对该控制方案从硬件设计和算法上实现。结果表明所研发的动镜运动控制系统具有足够的精度和实时性,能够保证FTIR光谱仪中干涉仪所需的准直性及动镜匀速性的要求。     

低曝光条件下遥感相机微振动量检测

针对搭载平台颤振对遥感相机成像的影响,利用辅助高速面阵CCD相机拍摄高帧频图像序列,通过像元合并来补偿曝光时间不足,增加图像的亮度、对比度和信噪比,同时结合一种区域选择算法来选择用于计算的图像区域,最后使用灰度投影算法对振动位移量进行估计.实验数据表明,提出的改进算法误差为一个像元,在准确性和稳定性方面均明显优于原始算法.     

Simulation of 12C+12C elastic scattering at high energy by using the Monte Carlo method

The Monte Carlo method is used to simulate the ¹²C+¹²C reaction process. Taking into account the size of the incident ¹²C beam spot and the thickness of the ¹²C target, the distributions of scattered ¹²C on the MWPC and the CsI detectors at a detective distance have been simulated. In order to separate elastic scattering from the inelastic scattering with 4.4 MeV excited energy, we set several variables: the kinetic energy of incident ¹²C, the thickness of the ¹²C target, the ratio of the excited state, the wire spacing of the MWPC, the energy resolution of the CsI detector and the time resolution of the plastic scintillator. From the simulation results, the preliminary establishment of the experiment system can be determined to be that the beam size of the incident ¹²C is φ 5 mm, the incident kinetic energy is 200-400 A MeV, the target thickness is 2 mm, the ratio of the excited state is 20%, the ight distance of scattered ¹²C is 3 m, the energy resolution of the CsI detectors is 1%, the time resolution of the plastic scintillator is 0.5%, and the size of the CsI detectors is 7 cm×7 cm, and we need at least 16 CsI detectors to cover a 0° to 5° angular distribution.