水浴法制备CdS薄膜产生的本征缺陷对光电学性质的影响

采用化学水浴沉积法(CBD)在钠钙玻璃衬底上制备硫化镉(CdS)薄膜,研究不同硫酸镉(CdSO_4)浓度下产生的本征缺陷对CdS薄膜光电学性质的影响。采用光致发光光谱、紫外-可见分光光度计及霍尔效应测试系统对薄膜的本征缺陷、光学及电学性质进行分析,发现CdS薄膜主要存在镉间隙(Cdi)及硫空位(VS)等本征缺陷,且VS随CdSO_4浓度的降低而逐渐减少。同时,VS缺陷的减少有利于薄膜透过率的提高,但在一定程度上降低了薄膜的电导率。根据透过率及其相关公式可知,半导体材料中透过率与电导率成e指数反比关系,适当减小薄膜的电导率可以使其透过率得到大幅度的提高,理论解释与实验结果相一致。     

Lateral stress-induced propagation characteristics in photonic crystal fibres

Using the finite element method, this paper investigates lateral stress-induced propagation characteristics in a photonic crystal fibre of hexagonal symmetry. The results of simulation show the strong stress dependence of effective index of the fundamental guided mode, phase modal birefringence and confinement loss. It also finds that the contribution of the geometrical effect that is related only to deformation of the photonic crystal fibre and the stress-related contribution to phase modal birefringence and confinement loss are entirely different. Furthermore, polarization-dependent stress sensitivity of confinement loss is proposed in this paper.     

The influence of strain-reducing layer on strain distribution and ground state energy levels of GaN/AlN quantum dot

This article deals with the strain distributions around GaN/AlN quantum dots by using the finite element method. Special attention is paid to the influence of Al_0.2Ga_0.8N strain-reducing layer on strain distribution and electronic structure. The numerical results show that the horizontal and the vertical strain components are reinforced in the GaN quantum dot due to the presence of the strain-reducing layer, but the hydrostatic strain in the quantum dot is not influenced. According to the deformation potential theory, we study the band edge modifications and the piezoelectric effects. The result demonstrates that with the increase of the strain reducing layer, the transition energy between the ground state electron and the heavy hole increases. This result is consistent with the emission wavelength blue shift phenomenon observed in the experiment and confirms that the wavelength shifts toward the short wavelength range is realizable by adjusting the structure-dependent parameters of GaN/AlN quantum dot.     

[NEt4][Mn(salophen)(H2O)2]2[Fe(CN)6]· H2O· CH3OH超分子化合物的合成和结构

室温下将 [NEt4 ]3[Fe (CN) 6 ]和 [Mn (salophen) (H2 O) (CH3OH ) ]ClO4 反应 ,得到了超分子化合物[NEt4 ][Mn(salophen) (H2 O) 2 ]2 [Fe(CN) 6 ]·H2 O·CH3OH (salophenH2 =双水杨醛缩邻苯二胺 ) ,并对其进行了晶体结构测定 .结果表明 ,该晶体属三斜晶系 ,空间群P1- ,晶胞参数a =1.2 15 0 ( 4)nm ,b =1.483 4( 6)nm ,c =1.662 5 ( 6)nm ,α =81.896( 7)° ,β =76.980 ( 8)° ,γ =81.12 0 ( 6)°,V =2 .872 ( 2 )nm3,Z =2 ,Dc=1.3 88g·cm-3.晶体的各部分间以氢键连接成网状超分子体系     

[Co(2,3-tri)(een)Cl][ZnCl4]配合物的合成及部分异构体的晶体结构测定

用过氧化物法合成、分离了[Co(2,3-tri)(een)Cl][ZnCl4](2,3-tri=N-(2-胺基乙基)-1,3-丙二胺,een=N-乙基乙二胺)体系中的部分异构体,解析了其中两异构体的晶体结构.其中晶体(Ⅰ)属单斜晶系,空问群p21/n,a=0.8611(4)nm,6=1.7906(9)nm,c=1.3374(7)nm,β=107.627(8)°,V=1.9653(16)nm3,Dc=1.713g·cm-3,Z=4,F(000)=1032,μ(MoKc)=27.43cm-1,R=0.0725,Rw=O.1798;晶体(Ⅱ)同属单斜晶系,空间群P21/c,a=0.9799(3)nm,b=2.6815(9)nm,c=0.8107(3)nm,β=107.595(6)°,V=2.0305(11)nm3,Dc=1.658g·cm-3,Z=4,F(000)=1032,μ(MoKa)=26.62em-1,R=0.0660,Rw=0.1536.两异构体中Co3+为六配位,其差异仅表现在二元胺(een)中乙基的取向不同.晶胞中含4个配合物阳离子,4个[ZnCl4]2-阴离子.在结构单元中对映体的比例为11.     

[Co(2,3-tri)(cmen)Cl][ZnCl4]配合物的合成及其两经式异构体的晶体结构

合成了[Co(2,3-tri)(cmen)Cl][ZnCl4](2,3-tri=N-(2-胺乙基)-1,3-丙二胺;cmen=1,2-二胺基丙烷)体系中的部分配合物异构体,解析了其中两异构体的晶体结构.其中晶体(Ⅰ)属单斜晶系,空间群P21/c,a=1.0211(2)nm,b=0.9208(2)nm,c=1.9511(4)nm,β=97.907(4)°,V=1.8161(7)nm3,Dc=1.803g@cm-3,Z=4,F(000)=1000.00,μ(MoKα)=29.66cm-1,R=0.0317,Rw=0.0923,晶胞中含4个配合物阳离子,4个[ZnCl4]2-阴离子;晶体(Ⅱ)属三斜晶系,空间群P1,a=0.90953(18)n,,b=0.9694(2)nm,c=1.1771(2)nm,α=110.669(4)°,β=92238(4)°,y=91.211(4)°,V=0.9697(3)nm3,Dc=1.750g@cm-3,Z=2,F(000)=52000,μ(MoKα)=27.84cm-1,R=0.0365,Rw=0.0975,晶胞中含2个配合物阳离子,2个[ZnCl4]2-阴离子及2个水分子.两异构体中Co3+为六配位,其差异仅表现在二元胺(cmen)中甲基的取向不同.在结构单元中对映体的比例为11.     

Ruthenium terpyridine complexes containing a pyrrole-tagged 2,2'-dipyridylamine ligand-synthesis, crystal structure, and electrochemistry

Ruthenium(II) terpyridine complexes containing the pyrrole-tagged 2,2'-dipyridylamine ligand PPP (where PPP stands for N-(3-bis(2-pyridyl)aminopropyl)pyrrole with the general formula [Ru(tpy)(PPP)X](n+) (1, X = Cl(-); 2, X = H(2)O; 3, X = CH(3)CN; tpy = 2,2':6',2"-terpyridine) have been synthesized and characterized by (1)H NMR, IR, UV-vis, mass spectrometry, and elemental analysis. 1 and 2 have been structurally characterized by X-ray crystallography. Both 1 and 2 were successfully immobilized onto glassy carbon electrode via anodic oxidation of the pyrrole moiety on the PPP ligand to give stable and highly electroactive polymer films. Cyclic voltammetric studies of 1 in acetonitrile revealed a Ru(III)/Ru(II) couple at 0.4 V vs Cp(2)Fe(+/0) initially, but another redox couple resulting from chloride substitution by acetonitrile developed at E(1/2) = 0.82 V upon repetitive potential scan. This ligand substitution was induced by the acidic local environment caused by the release of protons during pyrrole polymerization. The electropolymerization of 2 in aqueous medium allowed the observation of the formation of Ru(IV)═O species in polypyrrole film. As the film grew thicker, the size of the Ru(III)/(/)Ru(II) couple (E(1/2) = 0.8 V vs SCE at pH 1) of poly[Ru(tpy)(PPP)(OH(2))](n+) increased accordingly, whereas the growth of the Ru(IV)/Ru(III) couple (E(1/2) = 0.89 V vs SCE at pH 1) leveled off after the film had reached a certain thickness. The Pourbaix diagram of the E(1/2) of the Ru(III) /Ru(II) and Ru(IV)/Ru(III) couples vs pH of the electrolyte medium has been obtained. The resulting poly[Ru(tpy)(PPP)(OH(2))](n+) film is electrocatalytically active toward the oxidation of benzyl alcohol.     

A highly coarse-grained model to simulate entangled polymer melts

We introduce a highly coarse-grained model to simulate the entangled polymer melts. In this model, a polymer chain is taken as a single coarse-grained particle, and the creation and annihilation of entanglements are regarded as stochastic events in proper time intervals according to certain rules and possibilities. We build the relationship between the probability of appearance of an entanglement between any pair of neighboring chains at a given time interval and the rate of variation of entanglements which describes the concurrence of birth and death of entanglements. The probability of disappearance of entanglements is tuned to keep the total entanglement number around the target value. This useful model can reflect many characteristics of entanglements and macroscopic properties of polymer melts. As an illustration, we apply this model to simulate the polyethylene melt of C(1000)H(2002) at 450 K and further validate this model by comparing to experimental data and other simulation results.     

顶盖驱动流中胶束形态变化的耗散粒子动力学研究

利用耗散粒子动力学模拟方法研究了顶盖驱动方腔流条件下, 线性两嵌段共聚物胶束形态的变化. 结果表明弱的流场对胶束的形态影响不大, 但是在中等强度流场的作用下, 小胶束会融合并形成条状胶束, 而在很强的流场作用下, 胶束会被破坏而形成体积更小的球状胶束.     

高分子在受限稀溶液中的结构和动力学性质

利用平衡态及非平衡态耗散粒子动力学模拟方法, 分别研究了平衡态和流场作用下受限高分子在稀溶液中的链结构和动力学. 采用没有滑移和密度涨落的边界条件模拟纳米管道环境, 进而研究了高分子回转半径和扩散系数对受限强度及高分子与溶剂间相互作用的依赖关系. 在非平衡态模拟中, 分别考虑了Poiseuille和Couette两种流场. 研究发现, 在这两种流场作用下, 高分子都随着溶剂与高分子排斥作用的降低而向管道中心迁移. 在强流场下, 在Poiseuille流场中高分子密度呈现出双峰分布, 而在Couette流场中则呈现为单峰分布.