PHOTOCATALYTIC HYDROGEN EVOLUTION FROM WATER SPLITTING UNDER VISIBLE LIGHT IRRADIATION ON NOVEL PHOTOCATALYST FULLENES-PVP-ZN0.999NI0.001S

Fullerenes (C60/C70) linked up to Ni-doped ZnS through the medium of an amphalic polymer polyvinyl pyrrolidone (PVP) to form a new kind of photocatalyst for hydrogen evolution from aqueous Na2S/Na2SO3 solution under visible light irradiation, the photocatalytic activities of this novel photocatalyst C60/C70-PVP-Zn0.999Ni0.001S are 3-5 fold higher compared with that of precurse catalyst Zn0.999Ni0.001S. This result could be attributed to Schottky barrier layer built between C60/C70 and Zn0.999Ni0.001S due to the electro-negativity of C60 and characteristic of being used as a multiple electron acceptor. C60 or C60/C70, its moiety, with its low energy first excited singlet state, is a good energy acceptor and in addition readily accepts multiple electrons, making it a potential electron accumulate as we know, which could protect the separation between electrons and holes against combination. This is an important reason for the marked increase of amount of H2 evolution during the photocatalytic process for the composite system C60/C70-PVP-Zn0.999Ni0.001S.     

低压下酞菁裂解法制备定向碳纳米管阵列

在低压条件下以酞菁铁为原料, 采用独立双温控加热系统在石英玻璃基底上气相沉积制备了大面积准直性好和管径均匀的碳纳米管. 利用扫描电子显微镜(SEM/FESEM)和透射电子显微镜(TEM)研究了定向碳纳米管的生长形态和结构. 详细讨论了系统真空度、反应温度、气体流速及氢气和氩气的体积比例等参数对碳纳米管生长的影响, 并测试了该碳纳米管的场发射性能及超电容性能.     

谐振调幅压电石英晶体分子键裂型传感仪的研制北大核心CSCD

基于谐振调幅激励压电石英晶体开发了一种分子键裂型传感仪。该传感系统通过数字信号发生器DDS 9854产生频率可调的正弦波,激励9.98 MHz的压电石英晶体,经信号放大滤波后得到谐振频率。通过数控技术调节激励电压实现谐振调幅,以增大石英晶振表面的剪切动量。当调幅到一定程度会导致分子间键断裂,通过调幅电压值测定分子键的强度,可在数分钟内得到晶体表面的结合质量和结合强度的信息。使用了谐振调幅压电石英晶体分子键裂型传感仪检测了不同粒径的氨基纳米磁珠与金电极之间的相互作用,由频率信号得到磁珠在金电极上的结合量。通过不同谐振调幅电压激励石英晶体以甩脱电极表面的磁珠,由激励电压得到不同粒径的氨基纳米磁珠与金电极间的键裂力为2±0.5 nN。本仪器的研制为传感分子间的相互作用提供了一种新技术,可快速检测鉴别键的强度。     

数列

1.本单元知识点数列作为一种特殊的函数,是反映自然规律的基本数学模型,是高中数学非常重要的基础内容.又由于数列与函数、方程、不等式有着紧密而广泛的联系,可以用来考查学生对数学思想方法的理解以及综合运用知识的能力,因此它也是高考的一个重点.本单元学习重点包括:数列的概念,an与Sn之间的关系,等差数列的概念、通项公式与前n项和公式,等比数列的概念、通项公式与前n项和公式.本单元学习难点包括:递推数列的求解,数列     

单分子电导测量技术及其影响因素

Molecular electronics is an important field for the application of nanotechnologies with an ultimate goal of building functional devices using single molecules or molecular arrays to realize the same functionality as macroscopic devices. To attain this goal, reliable techniques for measuring and manipulating electron transfer processes through single molecules are essential. There are various techniques and many environmental factors influencing single-molecule electronic conductance measurements. In this review, we first provide a detailed introduction and classification of the current well-accepted techniques in this field for measuring single-molecule conductance. All available techniques are summarized into two categories: the fixed junction technique and break junction technique. The break junction technique involves repeatedly forming and breaking molecular junctions by mechanically controlling a pair of electrodes moving into and out of contact in the presence of target molecules. Single-molecule conductance can be determined from the conductance plateaus that appear in typical conductance decay traces when molecules bind two electrodes during their separation process. In contrast, the fixed junction technique is to fix the distance between a pair of electrodes and measure the conductance fluctuations when a single molecule binds the two electrodes stochastically. Both techniques comprise different application methods and have been employed preferentially by different groups. Specific features of both techniques and their intrinsic advantages are compared and summarized in Section 4.     

新型多取代Tr(o)ger's base衍生物的合成及其晶体结构

以邻氨基二苯甲酮为原料,经两分子环化缩合反应制得6,12-二芳基二苯并[b,f][1,5]二氮杂环辛四烯(2a~2d);2a~2d经LiAlH4还原制得6,12-二芳基-5,6,11,12-四氢二苯并[b,f][1,5]二氮杂环辛(3a~3d);3a~3d与醛(或酮)反应,合成了一系列新型的多取代Tr(o)ger's base衍生物(4a~4d和5a~7a),其结构经1H NMR, 13C NMR, HR-MS(ESI)和X-射线单晶衍射表征.通过分析架桥前后3a(CCDC: 1498564)和6a(CCDC: 1498555)的晶体结构,解释了该类化合物1H NMR中NCH质子及桥上取代基质子裂分的原因,并进一步证实了4~7为非C2轴对称结构.     

液体核磁共振中由分子间偶极耦合和分子内标量耦合共同作用后的谱图裂分模式

在高极化多自旋液体样品中,同时存在着分子间偶极（D）耦合和分子内标量（J）耦合,它们的共同作用产生了一些原来观测不到的分子间多量子相干信号。而且,信号的裂分模式与只存在J耦合的多自旋体系中观测到的多量子相干信号的裂分模式不同。本文从理论和实验上研究了这些禁阻的共振峰及其独特的裂分模式。为了比较验证,我们以I2S3+X自旋体系为例,结合使用选择和非选择性的射频脉冲序列来获得分子间双量子相干信号的五种裂分模式。进而归纳出对IpSq+Xk (p, q, k = 1, 2, 3,…)自旋体系普适的裂分模式规则。并指出,它们中如(1:0:-1)的裂分模式会放大J耦合裂分,使得J耦合常数的测量更精确,特别在J耦合常数很小或不均匀场中的J耦合常数的测量中具有诱人的应用前景。结果表明理论预测,计算机模拟和实验观测结果三者吻合的很好。     

钽的层裂实验数值模拟

 采用连续介质力学基唯象模型模拟分析了钽的平板撞击层裂行为。该模型包括了材料的非线性弹性（状态方程）、率相关塑性和孔洞的形核及生长等多种效应，并且采用一种对角隐式Runge-Kutta方法来求解本构率方程组，提高了热粘塑性本构关系计算的稳定性及精度。将数值模拟结果和相关实验数据进行了对比分析，结果表明，对于样品中的拉应力峰值明显高于材料层裂强度的实验（中、高速平板撞击实验），理论模型具有较好的预估能力，但对于临界层裂问题（低速平板撞击实验），该模型对材料损伤与失效过程的描述可能不够准确，需要进一步改进。     

中国散裂中子源简介

一、中子散射1932年,查德威克发现了中子,人们认识到原子核由带正电的质子和不带电的中子构成。中子的发现及应用是20世纪最重要的科技成就之一。当一束中子入射到所研究的对象上时,与研究材料中的原子核或磁矩发生相互作用,被散射出来,通过测量散射出来的中子能量和动量的变化