第一讲中子散射与散裂中子源

中子散射是研究物质微观结构和动态的理想工具之一,广泛地应用于凝聚态物质研究和应用的众多学科领域.散裂中子源能是新一代的加速器基脉冲中子源,能为中子散射提供高通量的脉冲中子.文章简明地介绍了中子散射的特点和它作为物质结构和动态探针的优越性,以及散裂中子源的基本原理、发展状况和多学科的应用优势.我国计划建设的散裂中子源CSNS中,靶站将由多片钨靶、铍/铁反射体和铁/重混凝土生物屏蔽体组成.质子束功率100kW下,脉冲中子通量约为2.4×1016n/cm2/s.第一期将设计建造高通量粉末衍射仪、高分辨粉末衍射仪、小角散射仪、多功能反射仪和直接几何非弹性散射仪等五台典型的中子散射谱仪,以覆盖大部分的中子散射研究领域.     

Preparation of Silver—Coated Polystyrene Composite Particles

We report a feasible approach to the preparation of monodispersed metal-shell composite microspheres based on a combination of surface reaction and surface seeding techniques. The method was implemented for coating polystyrene (PS) spheres with silver shell having a variable thickness by controlling the amount of reagents in the reaction procedure. These composite spherical particles in dimensions of the submicrometer range may become attractive building blocks for the creation of metallo-dielectric photonic band gap materials when they are organized into crystals.     

微全分析系统检测方法的研究进展

综述了不同类型的检测方法在微全分析系统的应用，并简述了各类型的检测方法的优缺点。引用文献92篇。     

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.     

含芴共轭高分子的合成、表征及性能研究——推荐一个高分子化学综合实验

推荐了一个高分子化学综合实验——含芴共轭高分子的合成、表征及性能研究。实验内容包括利用Sonogashira偶联反应合成共轭高分子,采用核磁共振和红外光谱等检测手段对其结构进行表征,并利用紫外-可见光谱、荧光和热重分析对其性能进行研究。本实验结合了高分子化学和聚合物仪器分析与表征的知识点,建议纳入高分子专业高年级综合实验课程。     

气相色谱与串联质谱联用检测血清中脱氢表雄酮

在晚期前列腺癌雄激素全阻断治疗最终导致前列腺癌雄激素非依赖性的转变过程中,肾上腺分泌脱氢表雄酮(DHEA)被认为是重要的诱因。本研究主要利用睾丸摘除(去势)大鼠模型,对血清中DHEA浓度进行测定。采用了气相色谱与串联质谱联用(GC-MS/MS)技术,建立了高灵敏度的测定大鼠血清中脱氢表雄酮(DHEA)的方法。样品经过甲醇沉蛋白,而后固相萃取提取血清中微量的DHEA,通过七氟丁酸酐(HF-BA)衍生,采用GC-MS/MS测定。对固相萃取条件、衍生化条件以及质谱测定条件进行优化。DHEA在0.1~100μg/L范围内线性良好,相关系数r为0.9996;在2~50μg/L浓度范围内,加标回收率在99%~106%之间;相对标准偏差小于5%。本方法灵敏度高,选择性好,可满足临床对于血清样品中DHEA的测定要求。对去势大鼠血清中DHEA测定结果表明,去势后DHEA明显上升。     

在线分子印迹-化学发光法对食品中苏丹红Ⅰ的测定

以苏丹红Ⅰ作模板分子,用悬浮聚合法制备出微米级苏丹红Ⅰ分子印迹聚合物并将其做成微固相萃取柱,直接安装在流动注射系统的八通阀上,对样品溶液中的苏丹红Ⅰ进行在线分离和富集;经甲醇和甲酸混合洗脱液（体积比2：1）在线洗脱后与酸性高锰酸钾发生化学发光反应。据此建立了在线分子印迹微固相萃取,高锰酸钾氧化苏丹红化学发光测定食品中苏丹红Ⅰ的新方法。结果表明,测定的苏丹红Ⅰ线性范围为1．0×10^-6～7．0×10^-4g／L,方法检出限（3仃）为3×10^-7g／L,11次平行测定1×10^-5g／L苏丹红Ⅰ溶液的化学发光强度相对标准偏差为2．0％。     

癌胚抗原毛细管电泳-化学发光均相免疫分析

建立了一种测定人血清中癌胚抗原的毛细管电泳-化学发光检测的均相免疫分析新方法.采用四苯硼钠增强luminol-H2 O2-HRP体系化学发光的原理,化学发光检测经毛细管电泳分离的,用辣根过氧化物酶(HRP)标记的癌胚抗体及免疫复合物.测定癌胚抗原的线性范围2.0～80.0 μg/L(R=0.9921),检出限为0.1 μg/L(绝对检出限为0.75 fg).     

两种磺胺类双核铜(Ⅰ)配合物的合成、结构和量子化学研究

分别将磺胺间甲氧嘧啶及磺胺噻唑与一水合乙酸铜(Ⅱ)在水(溶剂)热条件下反应,获得了其相应的金属配合物单晶。用元素分析、红外光谱、紫外光谱和X-射线单晶衍射对其结构进行了表征,结果表明两配合物均为双核化合物,中心Cu原子均采用二配位的直线型几何构型。用密度泛函理论方法对配合物进行了计算,结果表明配合物中金属Cu以+1价存在,这与晶体结构及光谱分析的结果一致,进一步的电荷布局分析结果与晶体结构中的配位情况相符,轨道密度等值面的分析推测配合物具有较好的抑菌活性。     

铝、铜、镍三元合金系中τ相的晶体结构变迁

A thorough investigation by means of X-rays has been carried out with the purpose to determine the nature of the ternary phase τ in Al-Cu-Ni alloys. In contrast with the conventional concept of alloy phase which is characterized by a definite type of crystal structure, systematic structure changes are found in the single phase field of τ which occupies quite an extensive area in the isothermal section of the phase diagram at room temperature. There are eight types of structures altogether, all derived from a basic rhombohedron with corners occupied by Al atoms and centres either occupied by the heavy atoms or remaining vacant. The basic rhombohedron is the building stone in the crystal architecture. By transforming the basic rhombohedron into a hexagonal prism in the usual way, all structures may be considered to be built up by stacking together a number of these hexagonal prisms along the triad. The transformation of one structure into another is quite systematic in the way that the number of the stacking stories in the unit cell increases according to the order 10, 11, 12, 13, 14, 15, 16, 17. The atomic arrangements in the different structures are closely related too, in the respect that they are all superstructures due to the presence of ordered vacancies in the rhombohedral centres.The principal factor controlling the formation of these structures has been fully considered. In view of the fact that the change of structure types follows closely with the content of Ni or Cu for alloys of constant Al content, the atomic size factor appears to be unimportant in the formation of these alloys. It has been shown that for alloy phases of the defect lattice type as the r-phase, the most fundamental factor is the average number of valency electrons per structural unit which is the basic rhombohedron in the present case. By assuming Hume-Rothery's valencies, the average number of valency electrons remains remarkably constant throughout the entire phase field, while the electron concentration varies with compositions. It has also been pointed out that for alloy phases where there is no unit cell change, the average number of electrons per structural unit is equivalent to the number of electrons per unit cell, and for alloy phase where there is no defect, this is in effect equivalent to the electron concentration.