水+3-甲基吡啶+溴化钠三元溶液临界跨接现象

采用折射率法在较宽温度范围内研究了溴化钠、3-甲基吡啶和水的临界质量分数分别为0.240、0.192和0.568体系的临界性质, 发现在近临界点临界指数为0.365, 与Fishe重整化值一致. 有效临界指数随着温度逐渐远离临界点, 从0.365下降到0.20左右, 但当排除了“正规项”的影响后, 展现出向平均场理论值0.5单调跨接的行为.     

647W灯泵浦大功率连续Nd:YAG激光器

 报道了一台灯泵浦大功率连续Nd:YAG激光器。对影响大功率固体激光器模块输出功率和光束质量的主要因素进行了理论分析，并提出提高激光器效率的措施：对聚光腔的形状、结构和材料以及冷却方式，泵浦灯的参数和材料，激光晶体的参数和镀膜进行优化设计，采用径向固定的谐振腔镜。该灯泵浦YAG晶体棒总体电光转换效率为4%，光束质量为22mm·mrad，输出功率647W。     

玻璃与玻璃化转变

玻璃与玻璃态的应用极其广泛。玻璃化转变是一种典型的非晶液-固转变,当转变发生时体系的结构并没有明显变化,因而我们无法将其归类于已有的任何相变类型。作为凝聚态物理和软物质领域的核心问题,玻璃化转变的研究已有近70年的历史。然而,时至今日,人们还是无法回答玻璃态的本质是什么这一基本问题。本文简述了玻璃态的性质以及伴随玻璃化转变发生的一些基本物理现象,并总结了半个世纪以来一些与玻璃化转变相关的理论,以期加深读者对玻璃及玻璃化转变的认识。     

可分解均衡函数均衡力度分析

证明了惩罚力度越大的均衡函数得到的变权向量构建的变权决策模型越偏于保守;而激励力度越大的均衡函数得到的变权决策模型越偏于乐观,这些结果与均衡函数的原始含义是一致的.最后,详细分析了几类常见的可分解均衡函数的惩罚力度和激励力度随着参数的变化情况.     

厚度诱导的YBa2Cu3O7-δ超导薄膜剩余应力及临界电流变化

本文通过脉冲激光沉积法制备了不同厚度(80nm、320nm、1000nm和2000nm)的YBa2Cu3O7-δ(YBCO)超导薄膜,对它们的剩余应力和临界电流特性进行了对比研究.通过系列的激光显微Raman光谱和磁化曲线测量分别获得了薄膜剩余应力和磁化临界电流密度(Jc)对薄膜厚度的依赖关系.结果显示超导薄膜内剩余应力越小,Jc越高.对于中等厚度的薄膜样品(320nm和1000nm),其膜内剩余应力较小,同时由其特征的磁通匹配场大小推知在该厚度范围内的样品具有较高的线性缺陷密度,从而显示出较高的Jc值.     

Chemical synthesis and characterization of manganese oxide coated Ni particles

Nanosized Ni particles with an average diameter of about 8 nm were prepared by reducing of NiCl 2 with sodium borohydride (NaBH 4 ) in aqueous solution. By moderate annealing in protective atmosphere, the composite grew up to be 15-20 nm particles. Both of the as-prepared and annealed Ni particles were coated by a layer of manganese oxide via decomposition reaction in aqueous KMnO4 solution. Hysteresis loops of as-prepared samples show a large increase in the magnetization with decreasing temperature and an unsaturated component at high magnetic field. In contrast, the ferromagnetic characteristics of annealed one are much stronger with large magnetization and coercivity. The thermomagnetic curves verified the coexistence of ferromagnetic Ni and antiferromangetic Mn oxide phases. But there exists no exchange bias behavior in the samples, even though the interface structure between the ferromagnetic Ni core and the antiferromagnetic manganese oxides has been distinctly formed. The absence of exchange bias probably originates from the weak ferromagnetic characteristic of Ni cores.     

离子液体电沉积CuInxGa1-xSe2薄膜

采用循环伏安法(CV)对离子液体Reline中三元CuCl₂+InCl₃+SeCl₄体系和四元CuCl₂+InCl₃+GaCl₃+SeCl₄体系的电化学行为进行了研究。研究表明,In³⁺并入三元CIS(Cu-In-Se)薄膜体系和Ga³⁺并入四元CIGS(Cu-In-Ga-Se)薄膜体系均有两种途径：一是发生共沉积,二是直接还原。利用电感耦合等离子体发射光谱(ICP)和扫描电镜(SEM)对沉积电势、镀液温度和主盐浓度对CIGS薄膜组成、镀层表面形貌的影响进行了测试,结果表明通过工艺参数的选择可以控制Ga/(Ga+In)和CIGS薄膜组成并得到化学计量比为Cu_1.00In_0.78Ga_0.27Se_2.13的薄膜。     

酒石酸铅锆的制备、表征及其燃烧催化作用

以酒石酸、硝酸氧锆和硝酸铅为原料,合成出了双金属盐酒石酸铅锆,采用有机元素分析、X射线荧光光谱和FTIR对其进行了表征。在程序升温条件下,利用TG/DTG、DSC、固相原位反应池/FTIR联用技术,研究了酒石酸铅锆的热行为和热分解机理,描述了酒石酸铅锆的热分解过程,分析得出其最终分解产物为ZrO2、PbO和C。利用螺压工艺制备了含酒石酸铅锆的推进剂样品,研究了酒石酸铅锆对双基系推进剂燃烧性能的影响,分析了其燃烧催化作用。结果表明,酒石酸铅锆对双基系推进剂的燃烧具有良好的催化作用,是一种高效的燃烧催化剂;酒石酸铅锆热分解的最终产物PbO是催化燃烧的主要活性物质,推进剂燃烧过程中形成了氧化铅-铅循环催化体系,而锆和碳则起辅助催化的作用。     

壳聚糖的改性及其纳米粒子的制备

通过壳聚糖上的氨基与硬脂酸和硫辛酸的羧基脱水缩合反应,将硬脂酸和硫辛酸接枝在壳聚糖上,引入的疏水性基团使修饰的壳聚糖具有两亲性。对修饰壳聚糖残留的自由氨基进行甲基化,使氨基的pKa值由6.6增加到6.8~7.1。修饰的壳聚糖在水介质中经超声分散即可形成纳米粒子,纳米粒子的Zeta电位为正值,说明修饰壳聚糖中残留的氨基和甲基化的氨基处于纳米粒子的表面。纳米粒子经二硫苏糖醇还原,然后经空气中的氧气氧化,在纳米粒子中形成二硫键交联结构。     

Nonisothermal crystallization and morphology of poly(butylene succinate)/layered double hydroxide nanocomposites

Biodegradable poly(butylene succinate) (PBS) and layered double hydroxide (LDH) nanocomposites were prepared via melt blending in a twin-screw extruder. The morphology and dispersion of LDH nanoparticles within PBS matrix were characterized by transmission electron microscopy (TEM), which showed that LDH nanoparticles were found to be well distributed at the nanometer level. The nonisothermal crystallization behavior of nanocomposites was extensively studied using differential scanning calorimetry (DSC) technique at various cooling rates. The crystallization rate of PBS was accelerated by the addition of LDH due to its heterogeneous nucleation effect; however, the crystallization mechanism and crystal structure of PBS remained almost unchanged. In kinetics analysis of nonisothermal crystallization, the Ozawa approach failed to describe the crystallization behavior of PBS/LDH nanocomposites, whereas both the modified Avrami model and the Mo method well represented the crystallization behavior of nanocomposites. The effective activation energy was estimated as a function of the relative degree of crystallinity using the isoconversional analysis. The subsequent melting behavior of PBS and PBS/LDH nanocomposites was observed to be dependent on the cooling rate. The POM showed that the small and less perfect crystals were formed in nanocomposites.