锐钛矿二氧化钛超细纳米晶的三声子互作用

本文通过对粒径为2.2-25.5nm的锐钛矿二氧化钛超细纳米晶在83-293 K温度范围内的变温拉曼光谱的研究,得到了三声子互作用对拉曼频率和线宽的贡献随粒径的变化关系。结果表明锐钛矿二氧化钛超细纳米晶的三声子相互作用随粒径减小而加强。     

Magnetic and Crystalline Microstructures of Fe-Pt-B Nanocomposite Ribbons

We investigate magnetic and crystalline microstructures of melt-spun (Fe0.675Pt0.325)100-xBx (x=12, 14, 16, 18,20) nanocomposite ribbons after optimal thermal treatment using a magnetic force microscope. The magnetic microstructures are characterized by darker spots adjacent to brighter ones in a sub-micro scale and in random distribution. It is found that the strength of the exchange coupling interaction between the crystals in the 10-100 nm scale, implied by the maximum value (δM)max of the Henkel plot, could be roughly described by the ratio of the average width of the magnetic spots w^- to the average crystal size D^- for the ribbons. Moreover, we find that the intrinsic coercivity jHc of the ribbons is sensitive to their crystal sizes, and the smaller D^-, the higher jHc. Finally, by using roughness analysis, the curve of the root mean square values (δФ)rms of the phase shift of the magnetic force images versus the boron content x is obtained, which is qualitatively consistent with that of the magnetization σ12 kOe of the ribbons versus x.     

排列形状及阵列数目对纳米导线阵列场发射性能的影响

为了进一步研究纳米导线阵列的排列形状以及阵列数目对其场发射行为的影响，利用镜像悬浮球模型对正方形以及六边形排列的纳米导线阵列的场发射行为进行计算与模拟，近似的得到纳米导线阵列的场发射增强因子满足如下的变化趋势：β=h/ρ(1/1+W)+1/2(1/1+W)²+3,其中h为纳米导线的高度，ρ为纳米导线的半径，W是以R为自变量的函数，R为纳米导线阵列的间距.结果显示纳米导线阵列的排列形状对其场发射性能的影响较小，而阵列间距则是影响场发射性能的关键因素：当R<R₀时，场发射增强因子随着阵列间距的减小而急剧减小；当R>R₀时，场发射增强因子基本不变，其中R₀为导线阵列场发射的最佳间距.进一步研究表明改变纳米导线阵列的数目基本不会改变阵列的场发射性能随间距的变化趋势，但是随着阵列数目的增加，R₀会有一定程度的减小，场发射增强因子也会降低. 关键词： 纳米导线 场发射 增强因子 阵列数目     

管式电极流体动力伏安法研究——Ⅳ.双管电极溶出-收集伏安法测定天然水中痕量铋

Johnson和Allen提出了一种称为收集的阳极溶出伏安法技术。首先将痕量金属离子电积在旋转环-盘系统中的盘电极上,再利用线性电位扫描使其溶出。溶出的金属离子在恒电位下以恒定的比例被收集在环电极上。由于在环电极上没有充电电流存在,因而得到的基线平坦,提高了信噪比,从而提高了分析的灵敏度。随后,Laser和Ariel,Schieffer和Blaedel等也进行过研究,并测定了铜、铅、锌和镉等痕量金属离子。     

示差脉冲阳极溶出伏安法测定痕量铋

采用自行研制的管式玻碳电极并以同位镀汞的示差脉冲阳极溶出伏安法测定痕量(?)。在盐酸介质中,铋离子浓度在2×10~(-9)—1×10~(-7)g/mL范围内与溶出峰电流呈良好的线性关系。实验结果与预期一致,应用于环境水样分析,结果令人满意。     

1,1,1-三[3-（2-苯并咪唑基）-2-氧杂丙基]丙烷镍配合物合成以及结构测定

合成了一个新的三脚架结构配体及其镍配合物的晶体。该晶体属单斜晶系， P2_l/n空间群，a = 1.2151(4) nm, b = 1.5535(5) nm, c = 2.1740(7) nm, β = 90.551(18)°, V = 4.103(2) nm~3, Z = 4, M_r = 834.03, R = 0.0556, wR = 0.1256, μ = 0.541 mm~(-1), F(000) = 1758。配合物中Ni与配体的三个N和 三个O构成六配位变形八面体结构。晶体中存在着分子间氢键，晶体结构依靠库仑 力和氢键作用而稳定。     

烟酸铬(Ⅲ)的配位结构与生物活性关系

合成了2种新型吡啶-3-羧酸(烟酸)铬(Ⅲ)螯合物,通过元素分析、热分析、红外光谱和电子光谱证明烟酸作为双齿配位体,形成具有3个六员环的螯合物Cr(Nic)3和具有2个六员环与2个H2O单体的混型配合物[Cr(Nic)2(H2O)2]Cl。通过使用效能等试验表明,在猪饲料中添加不同配位结构的烟酸铬均有明显提高饲料利用率、促进生长和显著提高机体对葡萄糖的清除率等作用。试验还表明,双齿配位的烟酸铬具有较高的生物活性、无毒、饲用后在肌体内无残留,作为饲料添加剂具有广阔的应用前景。     

Investigations of ionization-induced injection of laser wake field acceleration using phenomenological model

We develop a phenomenological model to investigate dynamics of ionization-induced injection. In the ＂bubble＂ regime of laser wakefield acceleration （LWFA）, it is found that there is an upper limit for laser intensity of ionization-induced injection. In the plane perpendicular to the laser polarization, when the laser pulse is linearly polarized, ionization-induced injected electrons exhibit a filamented structure and semi-coherent betatron oscillation.     

高分散在氮掺杂碳纳米管表面铂纳米粒子的高效甲醇电氧化性能

以氮掺杂碳纳米管（NCNT）为载体,利用掺杂氮原子的锚定作用,通过微波辅助乙二醇还原法方便地将Pt纳米粒子高分散地固载于NCNT表面,制得了Pt/NCNT系列催化剂,对催化剂制备规律、电催化甲醇氧化反应（MOR）性能及构效关系开展了系统深入的研究。结果表明,随Pt负载量在18.2%~58.7%（w/w,下同）范围增加,Pt纳米粒子的粒径在2.2~3.7 nm范围相应地逐渐增大。单位质量催化剂的MOR催化活性先增加后急剧减小,在负载量为47.8%时达到最大。Pt的质量比活性在中等负载量（27.6%~47.8%）区间出现高值平台。该变化规律源于Pt纳米粒子的MOR催化活性在3 nm前后的明显差异,即<3 nm时活性差,>3 nm时活性优异。高负载量（58.7%）时活性的急剧下降源于Pt纳米粒子因团聚引起的Pt利用率的降低。     

A 2D Wavy Parquet Architecture Based on the Biphenyl-3,3’,4,4’-tetracarboxylic Acid and Bis(2-benzimidazole)alkanes Ligands

A double-T-shaped ligand (H4BPTC) and bis(2-benzimidazole)alkanes as the spacers have been firstly used to direct the assembly of a 2D coordination polymer with wavy parquet network topology, [Zn(BPTC)0.5(H2C2EIm)(H2O)]n (1, C24H18ZnN4O5, Mr = 507.79, H4BPTC = biphenyl-3,3',4,4'-tetracarboxylic acid, H2C2EIm = 2,2'-(1,2-ethanediyl)-bis(1H-benzi- midazole), which was determined by single-crystal X-ray diffraction analysis. The crystal belongs to the monoclinic system, space group P21/n with a = 1.1844(5), b = 1.4019(5), c = 1.4026(5) nm, β = 108.359(5)°, V = 2.2104(15) nm3, Z = 4, Dc = 1.526 g/cm3, μ(MoKα) = 1.156 mm-1, F(000) = 1040, S = 1.038, the final R = 0.0427 and wR = 0.0793 for 3834 reflections with I > 2σ(I). The compound units are linked through BPTC ligands into a wavilness parquet 2D layer and further connected into a 3D framework via π-π packing interactions between the adjacent H2C2EIm ligands and weak N-H…O hydrogen bonding between uncoordinated carboxylate and the nitrogen atoms of H2C2EIm as well as the free water molecules.