四硫富瓦烯衍生物的银(Ⅰ)配位聚合物的合成与表征

在室温下,以丙酮为溶剂,三氟甲基磺酸银与4,5-二甲硫基-1,3-二硫代环戊烯-2-硫酮(C5H6S5)反应得到一个二维配位聚合物[Ag(C5H6S5)].CF3SO3.(CH3)2CO(1).单晶采用惰性溶剂扩散法培养.X-ray单晶衍射分析表明,1属于正交晶系,P212121空间群,晶胞参数:a=0.825 7(5)nm,b=0.972 1(6)nm,c=2.143(1)nm,V=1.720(1)nm3.在1中一个银离子与不同配体的三个硫原子配位,同时一个配体的两个硫原子参与和银离子配位,形成二维阶梯结构,在二维聚合物分子内存在较强的S…S相互作用,聚合物室温电导率为3.95×10-7S.cm-1,属于半导体.经过碘掺杂后化合物的电导率达到6.80×10-7S.cm-1.     

自仿集的势论和分析性质

研究了关于自仿集上电荷分布的势论及有关分析性质。指出电荷分布、势及其Fourier变换的构造性质;明确给出了三分Cantor集上二项分布及其矩、Fourier变换、势的具体表达式;并给出一些数值结果。     

本刊论文按SCI被引频次排序（前10名）表

据美国 ISI(科技信息研究所 )网络版刊载的 1985～ 2000年的文章引用情况,我们对在我刊发表的论文的有关情况进行了统计,并按作者总被引频次顺序整理出来 (见表 )。是否可以说,这个结果从一个侧面反映出,这些作者对我刊走向世界,扩大影响作出了突出的贡献。同时,我们也要对每一位向本刊投稿的作者、稿件评审人,以及关心、帮助过我们的各方人士表示衷心的感谢。我刊刊出文章按作者被引频次排序（前 10名）表(根据 1985～ 2000年 SCI网络版提供的数据 ) 作者总被引频次在我刊发表论文数名次作者总被引频次在我刊发表论文数名次赵新…     

小波分析方法在动态响应分析中的应用

小波分析是20世纪80年代后期发展起来的数学方法，作为—种全新的信号处理方法，它将各种不同频率成分组成混合信号分解到不同的频率段上，有效地用于信号滤波和信噪分离。在工程中常用的信号滤波方法一般有低通、带通、高通滤波，它们都只是提取信号某一频率段的成分，不能同时给出各个不同频率段的成分，因此所得到的信号其信息量不够完整。而小波变换能同时给出各个频率段的成分，其信息量是完整的。如图1所示。     

甲基橙在银镜上的表面增强拉曼光谱研究

利用表面增强拉曼光谱(SERS)技术研究了甲基橙的(MO)的SERS谱,对拉曼峰进行了指认,并给出了甲基橙在银镜上的吸附状态。     

无皂乳液聚合制备单分散核-壳聚丙烯酸微粒

核壳微粒;丙烯酸聚合物;无皂乳液聚合制备单分散核-壳聚丙烯酸微粒     

基于掺锡As2S8条波导的全光逻辑门研究

实验研究了掺锡As2S8条波导的光阻断效应,提出一种新型的基于掺锡As2S8波导的全光逻辑门方案,并试制了掺锡As2S8条波导全光逻辑门,实验结果显示该逻辑门具有良好的波形特性,表明该材料适合做全光逻辑门,具有一定的应用潜力.     

Novel Copper（Ⅱ） and Zinc（Ⅱ） 2-D Supramolecular Structures Based on Carboxylate and 1-Substitutedimidazole Mixed-ligands

Using the ligand bis(3-(1H-imidazol-1-yl)-1-phenylpropan-1-one) L, two novel com- plexes [CuL2(ph))]·H2O 1 and [ZnL2(tp)] 2 (ph = phthalic acid, tp = terephthalic acid) have been synthesized and their crystal structures were determined by single-crystal X-ray diffraction analysis. Crystal data for 1: triclinic, space group P1, a = 9.4300(17), b = 12.148(2), c = 13.721(2) , α = 109.620(2), β = 94.351(2), γ = 94.830(2)°, C32H30N4O7Cu, Mr = 646.14, V = 1466.2(4) 3, Z = 2, Dc = 1.464 g/cm3, μ(MoKα) = 0.801 mm-1, F(000) = 670, the final R = 0.0337 and wR = 0.0859 for 5122 observed reflections with I > 2σ(I). And those for 2: monoclinic, space group P2/n, a = 7.1866(11), b = 14.144(2), c = 14.407(2) , β = 101.427(2)°, C32H28N4O6Zn, Mr = 629.95, V = 1435.4(4) 3, Z = 2, Dc = 1.457 g/cm3, μ(MoKα) = 0.908 mm-1, F(000) = 652, the final R = 0.0438 and wR = 0.0821 for 2546 observed reflections with I > 2σ(I). In 1 and 2, ph or tp ligands bridge the six-coordinated copper(II) or four-coordinated zinc(II) ions forming 1D zigzag chains while L ligands act as the terminal monodentate ligand. It is noted that weak non-classical C–H···O plays the important and dominating roles in the formation of 2D supramolecular architectures of 1, but in 2 non-classical C–H···O and aromatic π-π stacking interactions are quite important and play dominant roles in the self-assembly of 2D supramolecular architectures.     

光气法制备酰氯的催化剂研究进展

酰氯是一类用途非常广泛的重要有机合成中间体,在工业上制备酰氯主要使用的氯化剂包括PCl3、PCl5、SOCl2、光气等,充分反应后通过过滤、蒸馏等工艺进行脱色提纯制得酰氯。光气法由于对环境污染较低,是目前最常用的方法。三光气可以分解成光气,其优良的物理、化学性质以及便捷的储存和运输条件是光气的最佳替代化学品。但由于光气活性较低,在使用过程中添加催化剂必不可少,本文将重点介绍目前光气法制备酰氯时所使用的各种催化剂及其性能。     

Strong near-field couplings of anapole modes and formation of higher-order electromagnetic modes in stacked all-dielectric nanodisks

We theoretically study the near-field couplings of two stacked all-dielectric nanodisks, where each disk has an electric anapole mode consisting of an electric dipole mode and an electric toroidal dipole (ETD) mode. Strong bonding and anti-bonding hybridizations of the ETD modes of the two disks occur. The bonding hybridized ETD can interfere with the dimer's electric dipole mode and induce a new electric anapole mode. The anti-bonding hybridization of the ETD modes can induce a magnetic toroidal dipole (MTD) response in the disk dimer. The MTD and magnetic dipole resonances of the dimer form a magnetic anapole mode. Thus, two dips associated with the hybridized modes appear on the scattering spectrum of the dimer. Furthermore, the MTD mode is also accompanied by an electric toroidal quadrupole mode. The hybridizations of the ETD and the induced higher-order modes can be adjusted by varying the geometries of the disks. The strong anapole mode couplings and the corresponding rich higher-order mode responses in simple all-dielectric nanostructures can provide new opportunities for nanoscale optical manipulations.