光源的选择对水溶性磺酸卟啉光催化对萘二酚类物质催化性能的影响

制备了水溶性磺酸卟啉(TPPS, TMPPS)及其铁配合物(FeTPPS). 以过氧化氢为氧源、 碘钨灯为光源, 水溶性磺酸卟啉可以高效光催化氧化1,5-萘二酚, 产物为5-羟基-1,4-萘二醌. 测定了卟啉的荧光量子产率及寿命, 分析了催化机理. 选择波长在350~650 nm区间内6个波段和功率在0~20 W区间内4种功率的光源, 探索了不同波段及功率的光源对卟啉光催化活性的影响. 研究结果表明, 不同波段的光源对卟啉光催化1,5-萘二酚的催化活性顺序为λ_380—385>λ_360—370>λ_580—585>λ_620—630>λ_492—577>λ_450—470, 该活性顺序与卟啉的紫外-可见吸收密切相关; 当使用相同波段光源时, 卟啉配体催化氧化1,5-萘二酚的反应速率常数与功率呈良好的线性关系; 卟啉铁配合物随着光源功率的增大, 其催化活性与光解程度有直接关系.     

CuInS2纳米晶的结构、形貌与光学性能研究

采用A-Pot法, 以乙酰丙酮铜[Cu(acac)₂]为铜源, 硬脂酸铟[In(St)₃]为铟源, 正十二硫醇(DDT)为硫源和稳定剂, 1-十八烯(ODE)为溶剂, 在250 ℃条件下, 反应50 min, 合成了CuInS₂粉体. 用X射线粉末衍射仪(XRD)、透射电子显微镜(TEM)、能量分散光谱仪(EDS)、X射线光电子能谱(XPS)等对粉体的结构、形貌、相组成进行表征. 结果表明: 产物为四角晶系的黄铜矿结构, 棒状CuInS₂纳米晶的直径为2 nm, 长约70 nm. 通过Z-Scan技术对分散在正己烷中CuInS₂纳米棒的三阶光学非线性进行测试, 在入射波长为770 nm的条件下, 得出三阶光学非线性折射率γ、三阶光学非线性吸收系数β以及三阶光学非线性极化率χ⁽³⁾分别为1.76×10^－17 m²/W, 7.95×10^－11 m/W和8.60×10^－12 esu.     

质子化g-C3N4/β-SiC复合材料的制备及光催化降解茜素红性能

分别采用热解法和溶胶-凝胶-碳热还原法合成了石墨相氮化碳(g-C₃N₄)和纳米级碳化硅(β-SiC), 通过浸渍-热处理法将两者复合并通过浓盐酸质子化, 分别制备了g-C₃N₄/β-SiC和质子化g-C₃N₄/β-SiC(P-g-C₃N₄/β-SiC)复合光催化剂. 利用X射线衍射(XRD)、 扫描电子显微镜(SEM)、 高分辨透射电子显微镜(HRTEM)、 傅里叶变换红外光谱(FTIR)、 X射线光电子能谱(XPS)、 紫外-可见漫反射光谱(UV-Vis-DRS)和光致发光光谱(PL)等对样品进行了表征. 结果表明, P-g-C₃N₄/β-SiC复合材料的比表面积增大, 光生电子-空穴对的复合几率降低, 光催化性能明显提高. 在光催化降解染料茜素红(ARS)研究中, 样品的可见光催化活性顺序为P-g-C₃N₄/β-SiC>g-C₃N₄/β-SiC>P-g-C₃N₄>g-C₃N₄>β-SiC. 其中P-g-C₃N₄/β-SiC在60 min内对ARS的降解效率高达99.9%, 符合准一阶动力学模型, 速率常数为0.0967 min ^-1, 且循环使用9次后, 光催化降解效率仍保持97.5%以上.     

用HRS技术研究CdS/Cd纳米粒子的二阶光学非线性

用新发展的超瑞利散射（HRS）技术（一种非相干的方法）研究了表面富镉的CdS纳米粒子的二阶非线性光学性质。结果表明每个纳米粒子的二次非线性极化率β值在10^-26esu量级,这是目前报导的具有最大β值的溶液物种之列。探讨了CdS纳米粒子产生二阶非线性的机制。认为纳米粒子大的比表面及表面缺陷结构对CdS纳米粒子的二阶光学非线性有很大影响。另外,双光子吸收诱导的共振增强作用亦可能贡献CdS纳米粒子的HRS信号,这种双光子共振吸收被其双光子荧光谱所证实。     

高β相聚偏氟乙烯基复合体系的制备及压电性能

为了提高聚偏氟乙烯(PVDF)的压电性能,需要寻找有效的途径来提高PVDF的电活性相(β相)含量。 通过水热法成功合成了Ag、ZnO以及二者复合(Ag-ZnO)的3种类型纳米粒子,并与PVDF共混形成PVDF复合薄膜。 通过表征PVDF复合材料的形貌,结晶性能和压电性能,可以发现Ag-ZnO复合纳米粒子的协同作用可以有效提高PVDF的结晶性能和压电性能。 此外,通过单轴拉伸可以使得所有PVDF膜的β相含量得到进一步提高,其中拉伸后的PVDF/Ag-ZnO纳米颗粒(P-C)的β相物质的量分数最高,达到70.0％,最佳的压电系数(d₃₃)达到了31.0 pC/N。     

氨基酸桥联手性双卟啉的二阶非线性光学性质研究

采用半经验量子化学PM3方法对系列氨基酸桥联双卟啉1, 2, 3, 4及其锌配合物进行了几何结构优化, 并用TDHF/PM3方法计算了其静态二阶非线性光学系数. 计算结果表明, L型-氨基酸桥联双卟啉及其锌配合物具有右手螺旋结构特征. 在电偶极近似下, 不同手性氨基酸侧链基团R对分子的总体二阶非线性光学系数β和βHRS的影响不大, 但对二阶非线性光学系数的手性分量βxyz却有显著影响. βxyz与螺旋结构参数r2ζ/L4成正比关系, 符合手性分子二阶非线性光学响应的单电子螺旋模型理论. β张量分析表明, 此类分子表现为以八极为主、 偶极为辅的多极分子, 卟啉环与锌离子的配位有利于增加二阶非线性光学响应的偶极分量和手性分量βxyz.     

基于二硫化钼/纳米金和硫堇/纳米金信号放大的雌二醇电化学适配体传感器

构建了一种新型的基于二硫化钼/纳米金和硫堇/纳米金信号放大的检测17β-雌二醇的电化学适配体传感器. 利用巯基自组装技术将17β-雌二醇的适配体探针DNA固定在二硫化钼/纳米金修饰玻碳电极表面, 与末端带巯基的部分互补DNA链杂交, 将硫堇/纳米金电化学指示剂自组装在杂交后的双链DNA上, 制备了17β-雌二醇电化学适配体传感器. 二硫化钼/纳米金复合材料增加了电极的有效表面积和DNA探针的固定量. 纳米金作为信号物质载体负载硫堇, 实现了电化学指示剂的信号放大. 加入目标物17β-雌二醇后, 目标物与适配体DNA特异性结合, 导致互补DNA链脱落, 双链上结合的硫堇/纳米金电化学指示剂数量减少, 电化学信号降低. 实验结果表明, 在1.0×10 ^-14~5.0×10 ^-12 mol/L范围内17β-雌二醇浓度与峰电流的线性关系良好, 检出限为4.2×10 ^-15 mol/L(S/N=3). 该传感器可望用于其它环境激素类物质的检测.     

不同晶型二氧化锰纳米棒催化氧化氯苯性能的研究

采用水热法分别合成了α-, β-, γ-MnO₂纳米棒, 使用X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、氢气程序升温还原(H₂-TPR)和X射线光电子能谱(XPS)等技术对三种晶型MnO₂纳米棒的结构和形貌进行了表征, 并以氯苯(CB)为探针考察了其催化活性和稳定性. 结果表明, 三种晶型MnO₂纳米棒在低温范围内均有较高的催化活性, 且活性顺序为α-MnO₂＞γ-MnO₂＞β-MnO₂. 此外, 还发现三种晶型MnO₂纳米棒比无定形MnO₂有更强的抗氯中毒能力. 在三种晶型MnO₂纳米棒中, α-MnO₂纳米棒催化氧化氯苯的活性最佳, 主要是由于该种MnO₂纳米棒含有丰富的晶格氧并且具有较强的可还原能力.     

聚(2-甲氧基-5-辛氧基)对苯乙炔/Tb4O7纳米复合材料的制备及其光物理性能研究

采用原位脱氯化氢缩合聚合法制备了聚(2-甲氧基-5-辛氧基)对苯乙炔/氧化铽(PMOCOPV/Tb₄O₇)纳米复合材料. 红外光谱证实了在Tb₄O₇表面的包覆层为PMOCOPV. 紫外-可见吸收光谱表明随着Tb₄O₇含量增加, PMOCOPV/Tb₄O₇的最大吸收峰发生红移且强度提高. 荧光光谱研究表明随着Tb₄O₇含量增加, PMOCOPV/Tb₄O₇的最大发射波长发生蓝移且强度提高, 荧光寿命得到增强, Tb₄O₇与PMOCOPV之间形成了光致电子转移体系, 使得π电子离域程度增加, 并且导致荧光量子效率提高. 根据E_g与入射光子能量hν的关系, 拟合了PMOCOPV/Tb₄O₇薄膜的光学禁带宽度, 发现随着Tb₄O₇含量增加, E_g减小. 采用简并四波混频方法测试它们的三阶非线性极化率χ⁽³⁾, 结果发现随着Tb₄O₇含量增加, PMOCOPV/Tb₄O₇纳米复合体的非线性光学响应逐渐增强, 这说明PMOCOPV与Tb₄O₇之间形成了分子间光致电子转移体系, 产生了复杂的分子间离域π电子非线性运动.     

β-环糊精的低临界溶解温度现象及其在有序纳米孔道片晶制备中的应用

将β-环糊精(β-CD)溶解于N,N-二甲基甲酰胺(DMF)中, 加热至140 ℃后有大量白色晶体析出. 扫描电子显微镜观察发现析出物为β-CD片状结晶. 红外光谱(IR)和核磁共振波谱(NMR)结果证明了片状结晶的化学结构与β-CD原料相同. 热重分析(TGA)和差示扫描量热(DSC)分析结果证明片状结晶的理化性质与β-CD原料相同. X射线衍射分析(XRD)测试结果表明, β-CD片晶的结晶结构与β-CD原料不同. 利用Diamond软件模拟了具有开通管道结晶结构的β-CD晶体的XRD谱图, 发现其与实测的β-CD片晶谱图基本相符, 说明β-CD片晶具有有序纳米开通管道结晶结构. 比表面积测试和酚酞吸附实验进一步证实β-CD片晶具有比β-CD原料更大的比表面积和更好的吸附性能.     

Modulation of the Second Order Nonlinear Optical Properties of Helical Graphene Nanoribbons Through Introducing Azulene Defects or/and BN Units

The current study has obtained excellent potential nonlinear optical(NLO) materials by combining density functional theory methods with sum-over-states model to predict the second order NLO properties of helical graphene nanoribbons(HGNs) through introducing azulene defects or/and BN units. The introduction of these functional groups deforms the pristine HGN (compression or tension) and enhances obviously the static first hyperpolarizability(<b₀>) of system by up to two orders of magnitude. The tensor components along the helical axis of HGNs play a dominant role in the total <b₀>. The azulene defects and the BN units polarize the pristine HGN to different degrees, and the azulenes and contiguous benzenes are involved in the major electron excitations with significant contributions to <b₀> but the BN units are not. The BN-doped chiral HGNs have good kinetic stability and strong second order NLO properties(6.84×10⁵×10^-30 esu), and can be a potential candidate of high-performance second order NLO materials. The predicted two-dimensional second order NLO spectra provide useful information for further exploration of those helicenes for electro-optic applications.     

NIR-Absorbing π-Extended Azulene: Non-Alternant Isomer of Terrylene Bisimide

The first planar π-extended azulene that retains aromaticity of odd-membered rings was synthesized by [3+3] peri-annulation of two naphthalene imides at both long-edge sides of azulene. Using bromination and subsequent nucleophilic substitution by methoxide and morpholine, selective functionalization of the π-extended azulene was achieved. Whilst these new azulenes can be regarded as isomers of terrylene bisimide they exhibit entirely different properties, which include very narrow optical and electrochemical gaps. DFT, TD-DFT, as well as nucleus-independent chemical shift calculations were applied to explain the structural and functional properties of these new π scaffolds. Furthermore, X-ray crystallography confirmed the planarity of the reported π-scaffolds and aromaticity of their azulene moiety.     

NIR‐Absorbing π‐Extended Azulene: Non‐Alternant Isomer of Terrylene Bisimide

The first planar π‐extended azulene that retains aromaticity of odd‐membered rings was synthesized by [3+3] peri‐annulation of two naphthalene imides at both long‐edge sides of azulene. Using bromination and subsequent nucleophilic substitution by methoxide and morpholine, selective functionalization of the π‐extended azulene was achieved. Whilst these new azulenes can be regarded as isomers of terrylene bisimide they exhibit entirely different properties, which include very narrow optical and electrochemical gaps. DFT, TD‐DFT, as well as nucleus‐independent chemical shift calculations were applied to explain the structural and functional properties of these new π scaffolds. Furthermore, X‐ray crystallography confirmed the planarity of the reported π‐scaffolds and aromaticity of their azulene moiety.     

Theoretical Studies on the Electronic Structure of Nano-graphenes for Applications in Nonlinear Optics

In this work, azulene is introduced into nano-graphene with coronene center to enhance the second-order nonlinear optical (NLO) properties. The sum-over-states(SOS) model based calculations demonstrate that dipolar contributions are larger than octupolar contributions to the static first hyperpolarizability(〈β₀〉) in most nano-graphenes except those with high symmetry(e.g., a C_2v nano-graphene has octupolar contributions Φ^J=3 up to 59.0% of the 〈β₀〉). Nano-graphenes containing two parallel orientating azulenes (i.e., Out-P and Out-P_s) have large dipole moments, while their ground state is triplet. Introducing B/N/BN atoms into the positions with a high spin density transfers the ground state of Out-P and Out-P_s to closed-shell singlet, and the Out-P_s-2N has a large 〈β₀〉 of 1621.67×10⁻³⁰ esu. Further addition of an electron donor(NH₂) at the pentagon end enhances the 〈β₀〉 to 1906.22×10⁻³⁰ esu. The two-dimensional second-order NLO spectra predicted by using the SOS model find strong sum frequency generations and difference frequency generations, especially in the near-infrared and visible regions. The strategies to stabilize the electronic structure and improve the NLO properties of azulene-defect carbon nanomaterials are proposed, and those strategies to engineer nano-graphenes to be semiconducting while maintaining the π-framework are exten-dable to other similar systems.     

Abnormal Nucleophilic Substitution on Methoxytropone Derivatives: Steric Strategy to Synthesize 5-Substituted Azulenes

Azulene is a non-alternant non-benzenoid aromatic system, and in turn, it possesses unusual photophysical properties. Azulene-based conjugated systems have received increasing interest in recent years as optoelectronic materials. Despite the routes available for the preparation of substituted azulene derivatives, there remain few methods that allow regioselective substitution on the seven-membered ring of azulenes due to the subtle reactivity difference among the various positions. This report explores the reactivity of substituted tropolones as the azulene precursors and also provides a new method to create 5-substituted azulenes. The reaction of cyanoacetate enolate with unsubstituted 2-methoxytropone affords azulene through the attack of the nucleophile on the C-2 center (normal pathway). We have observed that 3-substituted 2-methoxytropones undergo steric-guided nucleophilic addition at the C-7 center (abnormal pathway) to afford 5-substituted azulene derivatives. Based on this observation and DFT calculation, a new synthetic strategy is devised for the regioselective synthesis of 5-substituted multifunctional azulenes, which cannot be accessed by any other method.     

A comprehensive investigation of the interrelationships between spectroscopy and photochemistry and substituents of some azulenic derivatives

Several azulenic dyes, including six azulene hydrocarbons, two azulene aldehydes, and two olefinic azulenes, have been synthesized to survey their photophysics and photochemistry. These azulenes display S(2)-->S(0) emission, but with several differences. This is the most remarkable characteristic of the effect of orbital control on color and excited state properties of the azulenic compounds. This paper emphasizes how emission spectra and photochemistry of azulenic compounds are influenced by their chemical structure and solvent. The emission spectra of the azulene hydrocarbons suggest that their excited state properties can be controlled by their molecular structure and size. It was confirmed by emission and (1)H NMR spectroscopy that azulene monoaldehyde is protonated in a strong acid, such as trifluoroacetic acid (TFA). Photochemistry of styrylazulenes was observed during irradiation. Azulenic compounds are thermally stable and color tunable, and hence they are good candidates as non-linear optical materials. Based on their unique photochemical and photophysical characteristics, novel azulenic dyes can be constructed for different uses.     

Synthesis of 1‐(4‐thiazolyl)azulenes: Reactions of bromoacetyl‐substituted azulenes with thioamides,thioureas, and thiosemicarbazones

1‐(Bromoacetyl)‐3‐methylazulene (1a) and methyl 3‐(bromoacetyl)azulene‐1‐carboxylate (1b) reacted with thioamides 3a,b and thioureas 3c,d in boiling ethanol to give the corresponding (4‐thiazolyl)azulenes 4a‐d and 5a‐d in good yields, respectively. The reactions of dibromoacetyl‐substituted azulene (2) also gave (4‐thiazolyl) azulenes 5a‐d in lower yields and the azulene 2 was recovered. By heating compounds 5a‐d in 100% phosphoric acid, the ester group was eliminated to yield 1‐(4‐thiazolyl)azulenes 6a‐d. Compounds 1a,b reacted with thiosemicarbazones 7a‐f to afford [(2‐alkylidenehydrazino)thiazol‐4‐yl]azulenes 8a‐f and 9a‐f in moderate to high yields via their hydromides.     

刺激响应纳米碳杂化材料

碳纳米管和石墨烯是碳纳米材料的典型代表,其纳米尺度赋予了其优异的光、电、热以及机械性能。然而,这些碳纳米材料间存在较强的范德华力,导致其溶解性差,后续加工处理困难。为提高碳纳米材料的溶解性,通常利用聚合物或其它小分子物质对其进行修饰。而利用刺激响应性聚合物或化合物功能化碳纳米材料,不仅可以提高其溶解性,还可以赋予其环境刺激响应功能。本文主要综述了近年来利用温度、pH、光以及CO2响应聚合物或小分子化合物对碳纳米管和石墨烯进行共价键、非共价键修饰并赋予其环境刺激响应特性的方法、功能和相关应用,展望了修饰得到的纳米碳杂化材料的应用前景及下一步发展方向。     

三联噻吩基查尔酮衍生物的线性光学性质和超快非线性光学响应北大核心CSCD

以α-三联噻吩甲醛为原料,与3种二氯苯乙酮发生Claisen-Schmidt缩合反应,合成了3种含有三联噻吩基的查尔酮衍生物:1-(α-三联噻吩-2-基)-3-(2,4-二氯苯基)丙烯酮(a)、1-(2,5-二氯苯基)-3-(α-三联噻吩-2-基)丙烯酮(b)和1-(3,4-二氯苯基)-3-(α-三联噻吩-2-基)丙烯酮(c)。借助核磁共振波谱仪(^(1)H NMR、^(13)C NMR)和液-质联用谱仪(LC-MS)对其结构进行了表征;采用Z-扫描技术(600 nm,180 fs)测定了3个化合物的非线性光学吸收性能;运用含时密度泛函理论(TD-DFT)方法计算了它们的极化率(α_(0))、静态第一超极化率(β_(0))、振子强度(f_(0))、跃迁能(ΔE)、基态和最主要激发态之间的偶极矩差(Δμ)、最主要激发态的主要组成、最高占据分子轨道(HOMO)和最低空分子轨道(LUMO)之间的能隙,同时测定了它们的线性光学性质。结果表明,化合物c的紫外吸收波长、荧光发射波长、热稳定性、极化率均最大;化合物a—c均存在分子内电荷转移现象,非线性吸收均为双光子吸收,化合物a、b还有五阶非线性吸收,它们均表现出超快非线性光学响应,可作非线性光学研究备选材料。     

Theoretical approach to the out-of-plane deformation of 1,3-disubstituted azulenes

Computational calculations at B3LYP/6-311++G(d,p) and MP2/6-311++G(d,p) levels were employed to analyze the structure and conformation of 1,3-bis(4-bromophenyl)azulene (1), 1,3-bis(2-thienyl)azulene (2), and 1,3-bis(2-pyrrollyl)azulene (3) in order to rationalize the out-of-plane deformation found in the azulene cores of 1 and 2 in the crystalline state, whereas compound 3 shows a totally planar azulene moiety. Our results indicate that 1,3-disubstituted azulenes possess two almost equally stable and easily convertible minimum energy conformers, which differ in the relative orientation of the substituent groups and in the planarity degree of the azulene core. An absolute planarity index (P) is introduced to quantify the out-of-plane distortion found in the azulenes under study. The aromaticity of minimum energy conformers was evaluated by means of geometric (HOMA), magnetic (NICS), and energetic (the frequency of the lowest out-of-plane vibration, ν_min) aromaticity indicators, which suggest that compound 3 possesses the most aromatic azulene core within the group. Calculated molecular dipole moments suggest that the conformation of 1,3-disubstituted azulenes in the crystalline state can be explained in terms of electrostatic intermolecular interactions rather than relative stability of planar and non-planar conformers.