液态低沸点气体的表面张力

利用双毛细管法测定了液氮沸点温度下液氮的表面张力。用非线性方程γ=γ0(1-T/TC)n描述了液态N2、O2、Ar、Xe、H2、Ne、He、F2和Kr的表面张力与温度的关系,并采用一元线性回归的方法拟合了上述各流体的参数γ0和n,准确度高于文献值,说明方程能正确表达表面张力与温度的关系。这些数据有利于对上述低沸点气体进行准确的热力学计算。     

超高效液相色谱-四极杆飞行时间质谱测定动物饲料中3种巴比妥类违禁药物

建立了超高效液相色谱-四极杆飞行时间质谱(UPLC-O-TOF-MS)快速检测动物饲料中违禁添加的巴比妥、苯巴比妥和异戊巴比妥3种药物的分析方法.样品经甲醇振荡提取,再用C18固相萃取柱净化处理后,采用UPLC-O-TOF-MS分析检测.在电喷雾负离子模式和飞行时间模式下,以20mDa为提取离子窗口,输入各化合物的精确...     

一类趋化性生物模型行波解的存在性

我们研究了一类趋化性(Chemotaxis)生物模型在不同情形下行波解的存在性.对D=0的一些情形,利用相平面分析的方法得到了行波解存在的充分必要条件;对D>0的一些情形得到了行波解的存在性,改进了Nagai和Ikeda原有的结果.     

线性互补问题与多目标优化

本文研究了求解线性互补问题的一类新方法:把线性互补问题转化为多目标优化问题,利用多目标优化有效解的定义,给出了零有效解的概念;进而获得多目标优化问题的零有效解就是线性互补问题的最优解.最后给出了有解、无解线性互补问题,并分别把这些问题转化为多目标优化,采用极大极小方法求解转化后的多目标优化问题.数值实验结果表明了该方法的正确性和有效性,完善了文献[19]的数值结果.     

磁场对La2-x-yNdySrxCuO4体系电荷条纹相的影响

最近的研究结果表明在La2-x-yNdySrxCuO4体系中,静态电荷条纹的形成以及动态电荷条纹的运动都和晶格有一定的耦合.基于此,我们通过超声衰减测量研究了磁场对La2-x-yNdySrxCuO4(x=0.12, y=0, 0.4 and x=0.04, y=0)体系中电荷条纹的影响.对La1.48Nd0.4Sr0.12CuO4,我们发现70 K附近对应于静态电荷条纹形成的超声衰减峰以及此温度以下超声声速的异常硬化在零场和14T的强磁场下基本没有变化,说明静态电荷有序非常稳定,磁场对其没有影响.但是对La1.88Sr0.12CuO4样品,由于超导电性占主导地位,静态电荷序的形成被压制在很低的温度(10 K以下).我们发现低温下的超声衰减峰及声速硬化随磁场的增加而逐渐向高温方向移动,同时低温下的声速硬化加强.这意味着磁场能够钉扎La1.88Sr0.12CuO4中的动态电荷条纹.这一实验结果为La系超导体中静态电荷有序与超导电性之间的竞争提供了了进一步的证据.随着磁场的加强,超导序逐渐被压制,静态电荷序得以显现.La1.96Sr0.04CuO4的超声衰减特性测量结果显示,在团簇玻璃态下由于作为团簇畴壁的电荷条纹的运动而导致的超声能量损耗不随磁场发生变化.     

CdSe:Nd纳米晶及CdSe:Nd@SiO2核壳结构的合成及发光性能

利用有机相法合成Nd³⁺掺杂CdSe纳米晶（CdSe∶Nd）,通过X射线粉末衍射（XRD）、透射电镜（TEM）、紫外吸收光光谱及荧光光谱表征,证明Nd³⁺已经成功掺入到CdSe的晶格中。与纯CdSe纳米晶相比,CdSe∶Nd纳米晶的结构仍为立方晶型,且形貌近似球形,均匀分散,粒径约为2~4 nm。紫外吸收峰和荧光发射峰都发生红移,而且掺杂后的CdSe∶Nd纳米晶量子产率也提高,这可能是由于掺杂Nd³⁺引入了新的杂质能级,带隙减小。为了实现CdSe∶Nd纳米晶的可加工性和功能性,通过微乳法合成SiO₂壳包覆的CdSe∶Nd纳米球（CdSe∶Nd@SiO₂纳米球）,CdSe∶Nd@SiO₂纳米球呈均匀球形,直径约为100~115 nm,并且包壳后的CdSe∶Nd@SiO₂纳米球发射峰（581 nm）与CdSe∶Nd纳米晶（598 nm）相比,发光强度提高且发射峰蓝移,蓝移约为17 nm,可能是因为SiO₂壳可以减少纳米晶表面的非辐射跃迁以及改善表面缺陷导致的。     

Co-Ni合金纳米线有序阵列的制备与磁性研究

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分位点函数的光滑非参数估计的BAHADUR表示

文中对分位函数给出了具有更广泛应用的光滑分位估计,证明了该光滑分位估计的逐点和一致的Bahadur强表示定理;并由此结果推导了估计的重对数律,强逼近等深刻结果。     

STOCHASTIC LINEAR QUADRATIC OPTIMAL CONTROL PROBLEMS WITH RANDOM COEFFICIENTS

61. IntroductionLet (fi, F, P, {R}tZo) be a complete filtered probability space on which a standard onedimensional Brownian motion w(') is defined such that {R}tZo is the natural filtrationgenerated by w(.), augmented by all the p-null sets in i. We consider the following stateequationwhere T E T[0, TI, the set of all {R}tZo-stopping times taking values in [0, T], (E sigLlt (fi;IR"); A, B, C, D are matrix-valued {R}tZo-adapted bounded processes. In the above, u(.) EU[T, T]gLI(T, T…     

Piezoelectric resonators with mechanical damping and resistance in current conduction

A novel design method for high Q piezoelectric resonators was presented and proposed using the 3-D equations of linear piezoelectricity with quasi-electrostatic approximation which include losses attributed to mechanical damping in solid and resistance in current conduction. There is currently no finite element sofware for estimating the Q of a resonator without apriori assumptions of the resonator impedance or damping. There is a necessity for better and more realistic modeling of resonators and filters due to miniaturization and the rapid advances in frequency ranges in telecommunication. We presented new three-dimensional finite element models of quartz and barium titanate resonators with mechanical damping and resistance in current conduction. Lee, Liu and Ballato’s 3-D equations of linear piezoelectricity with quasi-electrostatic approximation which include losses attributed to mechanical damping in solid and resistance in current conduction were formulated in a weak form and implemented in COMSOL. The resulting finite element model could predict the Q and other electrical parameters for any piezoelectric resonator without apriori assumptions of damping or resistance. Forced and free vibration analyses were performed and the results for the Q and other electrical parameters were obtained. Comparisons of the Q and other electrical parameters obtained from the free vibration analysis with their corresponding values from the forced vibration analysis were found to be in excellent agreement. Hence, the frequency spectra obtained from the free vibration analysis could be used for designing high Q resonators. Results for quartz thickness shear AT-cut and SC-cut resonators and thickness stretch poled barium titanate resonators were presented. An unexpected benefit of the model was the prediction of resonator Q with energy losses via the mounting supports.