8-羟基喹啉快速共沉淀分离富集原子吸收光谱法测定啤酒中的Cu和Pb

研究了用8-羟基喹啉-Mg(Ⅱ)共沉淀体系,以Mn(Ⅱ)为内标,快速共沉淀分离富集啤酒中的铜和铅,并用火焰原子吸收光谱(FAAS)测定的方法。共沉淀受pH值、载体镁和内标锰用量的影响。结果显示在pH为9的条件下,能够定量共沉淀试样中的铜和铅。当试液为100 mL时,方法的检出限分别为铜6.28×10-3 μg·mL-1,Pb 2.26×10-2 μg·mL-1回收率为97.6%～103.0%,基本消除了基体干扰,取得了较为满意的结果。该方法无需收集全部沉淀,与传统的共沉淀方法比较,克服了收集沉淀费时的缺点。方法快速、简便、重现性好。     

BeH，BeD，BeT分子基态(X2Σ+)的结构与势能函数

采用量子力学从头算方法，运用二次组态相互作用QCISD(T)/aug-cc-pVTZ和电子相关单双耦合簇CCSD(T)/6-311++G(3df，2pd)研究了BeH，BeD，BeT分子基态的结构与势能函数，计算出了这些分子的光谱数据(ω_e，ω_eχ_e，B_e，α_e，D_e)，结果与实验光谱数据吻合较好.这表明上述分子基态的势能函数可用经修正的Murrell-Sorbie+c₆函数来表示. 关键词： BeH BeD BeT分子基态 分子结构 势能函数     

ICP-AES测定Ni-Cr合金在人工唾液中析出的Ni离子

在模拟口腔环境下用人工唾液浸泡Ni-Cr桥,150h后采用ICP-AES测定Ni-Cr桥在人工唾液中的Ni离子析出量.镍在0.01-7.5μg/mL内有良好的线性关系,相关系数为0.9998;方法检出限为0.0059μg/mL;标准加入法测定镍的回收率为92.3%-99.8%.     

基于SRLG不相关的共享保护算法的研究

通过对共享保护算法的深入分析,使用K条最短路和迭代思想的方法,提出了两种共享风险链路组不相关的共享保护算法,并在仿真平台上对两种算法的性能进行了仿真.KWFF算法借鉴了传统的K条最短路策略,并且在每一个波长平面上,都对新到业务进行了K条工作路由的计算,极大挖掘了网络中潜在的波长资源.而IFF算法由于引入了迭代的思想,避免了共享风险链路组问题中,所特别有“陷阱”问题的出现,并且利用两套权重计算公式,在计算工作路由和保护路由的时候,充分考虑了网络资源的实时变化情况.通过仿真数据可以看到,与以往算法相比,KWFF和IFF算法大大降低了网络阻塞率,并且提高了网络资源的使用效率.     

光信息科学与技术专业的建设

就光信息科学与技术专业建设的专业定位、课程设置、学生毕业后的去向等问题发表了个人的看法。介绍了在这方面的一些做法,提供了有关数据,可供同类专业的建设参考。     

太阳能甲醇分解吸收-反应器研制与实验研究

利用中温太阳能为甲醇分解的吸热反应供热,可以将中温太阳能转化为合成气燃料的化学能,同时提高燃料热值和太阳能的可用性,还可以实现太阳能与化石燃料的互补.本研究提出了太阳能热化学系统的一体化设计原则,建立了综合考虑太阳能集热、反应动力学和反应器结构参数的太阳能甲醇分解反应器的理论分析模型,并首次研制了5 kW热功率的抛物槽式太阳能甲醇分解一体化实验装置.太阳能甲醇分解的实验结果表明太阳能集热器可以为甲醇分解提供200～300 ℃的反应温度,在辐照300～800 W/m2,甲醇进料量为0.5～4l/h条件下,甲醇转化率可以达到50%～95%,投射到吸收-反应器上的太阳能转换为燃料化学能的效率可以达到30%～60%,具有良好的甲醇分解和太阳能转换性能.研制的实验装置体现了一体化设计特征,同时理论分析结果与实验结果也具有很好的一致性.本文研究成果将为开拓太阳能与化石能源互补的能量系统提供理论支撑和实验数据.     

评论:“边界振动的微腔中的二能级原子”

<正>在曲照军等的文章中[1]作者声称他们能够解决腔场影响原子问题.在此我们显示出既然他们用于得到相互作用表象的哈密顿的变换不完备所以他们没有解决该问题.我们知道此相互作用的哈密顿量可表示为(h=1)H=ωa■a+ωmb■b+ω0/2σz+g1(a■σ_+σ+a)+g2a■a(b■+b),(1)这里a和a■是单模量子化场的产生与湮灭算符,而b和b■为量子谐振子的产生与湮灭算符,g1是单模辐射场与原子的乡耦合系数,g2是单模辐射场与振动边界的耦合常数.曲照军等人把哈密顿量(1)分解成自由和相互作用两个哈密顿量H=H0+HI.这里     

Theoretical study of stereodynamics for the N+H2/D2/T2 reactions

The effects of isotopic variants on stereodynamic properties for the title reactions have been investigated using a quasi-classical trajectory method based on the first excited state NH2（I^2A＇） potential energy surface [Li Y Q and Varandas A J C 2010 J. Phys. Chem. A 114 9644]. The forward–backward symmetry scattering of the differential cross section can be observed, which demonstrates that all these reactions follow the insertion mechanism. Three angle distribution functions P（θr）, P（φr）, and P（θr, φr） with different collision energies and target molecules H2/D2/T2 are calculated. It is shown that the product rotational angular momentum is not only aligned, but also oriented along the direction perpendicular to the scattering plane. The title reaction is mainly governed by the ＂in-plane＂ mechanism through the calculated distribution function P（θr, φr）. The observable influences on the rotational polarization of the product by the isotopic substitution of H/D/T can be demonstrated.     

Fluorescence lifetime imaging of molecular rotors to map microviscosity in cells

Fluorescence liftime imaging （FLIM） of modified hydrophobic bodipy dyes that act as fluorescent molecular rotors shows that the fluorescence lifetime of these probes is a function of the microviscosity of their environment. Incubating cells with these dyes, we find a punctate and continuous distribution of the dye in cells. The viscosity value obtained in what appears to be endocytotic vesicles in living cells is around 100 times higher than that of water and of cellular cytoplasm.Time-resolved fluorescence anisotropy measurements also yield rotational correlation times consistent with large microviscosity values. In this way, we successfully develop a practical and versatile approach to map the microviscosity in cells based on imaging fluorescent molecular rotors.     

Van der Pauw Hall Measurement on Intended Doped ZnO Films for p-Type Conductivity

A Van der Pauw Hall measurement is performed on the intended doped ZnO films （Na doped ZnO） grown by using the molecular beam epitaxial method. All as-grown samples show n-type conductivity, whereas the annealed samples （annealing temperature 900℃） show ambiguous carrier conductivity type （n- and p-type） in the automatic Van der Pauw Hall measurement. A similar result has been observed in Li doped ZnO and in as-doped ZnO films by other groups before. However, by tracing the Hall voltage in the Van der Pauw Hall measurement, it is found that this alternative appearance of both n- and p-type conductivity is not intrinsic behavior of the intended doped ZnO films, but is due to the persistent photoconductivity effect in ZnO. The persistent photoconductivity effect would strongly affect the accurate determination of the carrier conductivity type of a highly resistive intended doped ZnO sample.