钛掺杂对ZnO∶Ti透明导电薄膜性能的影响

以不同钛掺杂含量的氧化锌陶瓷靶作为溅射源材料,采用射频磁控溅射工艺在玻璃基片上沉积了Ti掺ZnO(TZO)透明导电薄膜,通过XRD、XPS、分光光度计和霍尔效应测试系统,研究了钛掺杂含量对TZO薄膜微观结构和光电特性的影响.结果表明:所有TZO薄膜均为六角纤锌矿结构,并且具有(002)择优取向,钛掺杂含量对薄膜性能具有明显的影响.当钛掺杂含量为3wt;时,TZO薄膜的结晶质量最好、可见光平均透过率最高、电阻率最低、品质因数最大(748.15 S/cm),具有最佳的光电综合性能.TZO薄膜的光学带隙随钛掺杂含量增加而单调增大.     

不同形状的钨酸钡纳米粒子的合成

不同形状的钨酸钡纳米粒子的合成;微乳液;钨酸钡;纳米粒子;十二胺;十一烯酸     

核壳乳液在电解质作用下的破乳过程

核壳乳液在电解质作用下的破乳过程;分光光度计;核壳乳液;电解质;乳液破乳     

Synthesis and Properties of a Heteronuclear Ag(Ⅰ)/Ni(Ⅱ) Complex

A complex, Ni (en)2 Ag3 (CN) 5 (en = ethylenediamine), was obtained through the reaction of [Ag (CN) 2] -units with Ni Ⅱ -diamine cation [Ni (en)2] 2 , and the structure was determined by single crystal X-ray diffraction. It is indicated that the complex has a 3D architecture through the silver-silver interactions and the bridging cyano groups. This complex displays interesting luminescent properties caused by argentophilicity at room temperature in solid state.     

Antikaon Condensation and In-medium Kaon and Antikaon Production in Protoneutron Stars

Antikaon condensation and kaon and antikaon production in protoneutron stars are investigated in a chiral hadronic model （also referred to as the FST model in this paper）. The effects of neutrino trapping on protoneutron stars are analyzed systematically. It is shown that neutrino trapping makes the critical density of K^- condensation delay to higher density and fifo condensation not occur. The equation of state （EOS） of （proto）neutron star matter with neutrino trapping is stiffer than that without neutrino trapping. As a result, the maximum masses of （proto）neutron stars with neutrino trapping are larger than those without neutrino trapping. If hyperons are taken into account, antikaon does not form a condensate in （proto）neutron stars. Meanwhile, the corresponding EOS becomes much softer, and the maximum masses of （proto）neutron stars are smaller than those without hyprons. Finally, our results illustrate that the Q values for K^＋ and K^- production in （proto）neutron stars are not sensitive to neutrino trapping and inclusion of hyperons.     

Error Thresholds in Single-Peak Gaussian Distributed Fitness Landscapes

Based on the Eigen and Crow-Kimura models with a single-peak fitness landscape, we propose the fitness values of all sequence types to be Gausslan distributed random variables to incorporate the effects of the fluctuations of the fitness landscapes （noise of environments） and investigate the concentration distribution and error threshold of quasispecies by performing an ensemble average within this theoretical framework. We find that a small fluctuation of the fitness landscape causes only a slight change in the concentration distribution and error threshold, which implies that the error threshold is stable against small perturbations. However, for a sizable fluctuation, quite different from the previous deterministic models, our statistical results show that the transition from quasi-species to error catastrophe is not so sharp, indicating that the error threshold is located within a certain range and has a shift toward a larger value. Our results are qualitatively in agreement with the experimental data and provide a new implication for antiviral strategies.     

近红外漫反射光谱法测定整粒小麦单株蛋白质含量

应用近红外漫反射光谱技术(波长为1 100～2 498 nm,分辨率为2 nm),以整粒小麦为材料建立适合于小麦单株分析的蛋白质含量分析系统。首先选取籽粒蛋白质含量具有梯度差异的小麦样品,然后对样品扫描得到原始光谱信息,通过散射校正及数学处理来消除原始光谱噪声,最后分别采用多元线性回归、主成分分析法和偏最小二乘法法建立回归方程。结果表明,优化各项参数后,光谱经过标准乘性散射校正和一阶导数处理后,回归分析采用修正的偏最小二乘法(MPLS)得到的定标模型效果最佳。最终得到的预测方程定标相关系数(RSQ)、交叉验证标准误差(SECV)、交叉验证相关系数(1-VR)分别为0.94,0.42,0.87。数学模型经过验证样品集检验,预测相关系数达到0.88。该模型达到了快速、无损分析单株小麦的要求,非常适合于品质育种的早代选择。     

苯硫酚吸附在新型Ag-Au合金纳米粒子上的表面增强拉曼光谱研究

以柠檬酸钠同时还原制备的Ag-Au合金纳米粒子为种子,用盐酸羟胺进一步使其生长得到粒径为40～60 nm的新型Ag-Au合金纳米粒子,采用UV-Vis光谱和TEM对纳米种子和再生长后的纳米粒子分别进行表征。两种粒子的UV-Vis光谱均只观察到一个等离子体共振峰,其频率随金的摩尔分数(x_Au)增加而红移,且TEM图像表明这两种粒子的颜色均一,因此判断这两种粒子均为合金结构。以苯硫酚为探针分子,研究了该新型合金纳米粒子的表面增强拉曼光谱(SERS),结果表明吸附了苯硫酚的合金纳米粒子的紫外最大吸收峰红移,并在近红外区出现聚集体的吸收峰。在632.8 nm波长激发下,由于表面等离子体共振效应Au上的SERS信号最强,而合金纳米粒子上的SERS信号随x_Au增大而增强。     

KDP/DKDP晶体生长的研究进展

采用传统降温法,KDP晶体的生长速度一般在1～2 mm/d,DKDP晶体的生长速度甚至更慢,并且晶体的恢复区域较大,利用率低;而采用快速生长法,晶体的生长速度可以提高到20～50 mm/d,并且晶体的恢复区域小,利用率高.本文回顾了KDP/DKDP晶体生长的研究进展.并重点评述了KDP/DKDP晶体快速生长的研究进展,报道了近年来大尺寸、高质量KDP晶体的研究动态.