枝化二阶非线性发色团分子的合成及在聚合物体系中的电光性能

设计合成了一类以2-二氰基次甲基-3-氰基-4,5,5-三甲基-2,5-二氢呋喃(TCF)为受体、己氧基取代噻吩为π电子桥的新型有机非线性光学化合物, 并利用紫外光谱、红外光谱、核磁共振以及质谱对化合物分子结构进行了鉴定, 同时对此类化合物在有机聚合物体系中的电光性能进行了表征和研究. 结果发现, 该类发色团分子与聚合物相容性好, 电光活性高, 并且随着发色团分子在聚合物体系中浓度的升高, 聚合物体系的宏观电光活性也有所提高, 甚至当发色团的掺杂质量分数高达47.2%时, 体系的电光活性仍呈上升趋势, 显示了该发色团的静电相互作用得到了明显抑制. 此时测得聚合物体系的电光系数为30 pm/V(1310 nm).     

基于氢键的侧链型超分子电光聚合物的制备与表征

设计并制备了一种基于氢键的侧链型超分子聚乙烯基吡啶电光聚合物,非线性发色团与聚合物主链之间的氢键作用经红外光谱进行表征。采用氢键将发色团挂接到聚合物,可一定程度地抑制发色团分子的聚集,防止宏观相分离,实现发色团的高浓度掺杂。同时,利用超分子氢键作用挂接也可在一定程度上抑制发色团间的偶极-偶极相互作用力,测得此体系极化电光聚合物薄膜的最大电光系数为17.6 pm/V。     

一种新型二阶非线性光学功能分子及其交联聚氨酯材料的合成

合成了新型的含有偶氮和噻吩环的二阶非线性光学功能分子, 用红外光谱、紫外光谱、核磁共振和质谱确定了其结构; 制备了含有该功能分子的两种交联型聚氨酯聚合物薄膜, 当测量波长为1 064 nm时,  用Marker条纹法测得的二阶非线性光学系数d33值分别为80.6 pm/V(发色团的数密度为0.91×1020 Molecules/cm3)和20.1 pm/V(发色团的数密度为2.21×1020 Molecules/cm3); 聚合物Ⅱ的取向热稳定性达到了152 ℃.     

二阶非线性光学聚合物材料研究进展

在介绍非线性光学效应和聚合物极化原理的基础上,综述了非线性光学聚合物材料的研究进展。     

两种含偶氮苯共轭桥新型生色团分子的合成及性能

通过重氮化偶合反应和羟醛缩合反应合成了以偶氮苯为共轭桥、以2,2,3-三甲基-4-氰基-5-二氰基亚甲基-2,5-二氢呋喃为电子受体, 而给体分别为二甲氨基和二乙氨基的两种有机非线性光学生色团分子MFNC和EFNC. 利用IR、1H NMR和元素分析对分子的结构进行了表征. TGA和DSC测试发现, MFNC的热稳定性略好于EFNC, 其热分解温度最高达266 ℃. 通过测定两种材料在氯仿、丙酮和DMSO中的紫外-可见光谱, 用溶致变色法计算得到两种材料在激光波长为1064 nm处的二阶非线性品质系数μgβ, 对比发现EFNC的μgβ值高于MFNC, 其值达59706×10-48 esu(1 esu=3.34×10-10C).     

含有噻唑生色团的Y-型有机分子的二阶非线性光学性质

采用密度泛函理论(DFT)B3LYP/6-31G*方法优化了一系列含有噻唑生色团的Y-型有机杂环分子的几何构型, 在此基础上结合有限场(FF)方法和含时密度泛函理论(TD-DFT)对分子的非线性光学(NLO)活性和电子光谱进行计算分析. 结果表明, 这些分子具有A-π-D-π-A(A: 受体, D: 给体)结构, 分子基态偶极矩、极化率和二阶NLO系数(β)随支链共轭桥的增长及生色团共轭效应的增大而增大. 同时, 该系列有机杂环分子的二阶极化率总的有效值(βtot)与其前线分子轨道能级相关, 分子的前线分子轨道能级差越小, βtot值越大.     

含有咪唑生色团系列树型有机分子二阶非线性光学性质的密度泛函理论研究

应用密度泛函理论(DFT)B3LYP/6-31G*方法计算研究了系列树型含有咪唑生色团的有机分子的结构和非线性光学性质.计算结果表明:该系列分子具有A- -D- -A(A:受体,D:给体)结构,分子基态的偶极矩、极化率、二阶NLO系数( )随共轭链的增长及吸电子基的增强而增大;同时,前线轨道能级差值越小此类分子的二阶极化率总有效值( )越大.计算的吸收光谱显示此系列树型分子在低能区域247.79nm-419.87nm都有一个最强吸收,并且均是最高占据轨道与最低空轨道之间的跃迁.     

基于氢键作用结合的超分子聚合物

非共价键结合的超分子聚合物由于其特殊的结构及性能引起了广泛的关注。本文在介绍超分子化学、氢键及超分子聚合物的基础上,主要综述了以氢键为结合力的多重氢键作用、羧基（D）与吡啶基（A）作用以及氢键与其它非共价键协同作用形成的超分子聚合物体系,并对超分子聚合物的研究现状及前景进行了评述。     

基于氢键作用结合的超分子聚合物

非共价键结合的超分子聚合物由于其特殊的结构及性能引起了广泛的关注.本文在介绍超分子化学、氢键及超分子聚合物的基础上,主要综述了以氢键为结合力的多重氢键作用、羧基(D)与吡啶基(A)作用以及氢键与其它非共价键协同作用形成的超分子聚合物体系,并对超分子聚合物的研究现状及前景进行了评述.     

基于氢键作用结合的超分子聚合物

非共价键结合的超分子聚合物由于其特殊的结构及性能引起了广泛的关注。本文在介绍超分子化学、氢键及超分子聚合物的基础上,主要综述了以氢键为结合力的多重氢键作用、羧基(D)与吡啶基(A)作用以及氢键与其它非共价键协同作用形成的超分子聚合物体系,并对超分子聚合物的研究现状及前景进行了评述。     

以三聚茚为核的星型电子受体材料的合成、 表征与光伏性能

以高度平面共轭的烷基取代三聚茚为中心核, 以噻吩基团桥联, 在末端连接氰基茚酮作为拉电子基团, 设计合成了一类星型受体分子2,2',2″-{[(5,5,10,10,15,15-己基-10,15-二氢-5H-二茚[1,2-a：1',2'-c]芴-2,7,12-三基)三(噻吩-5,2-二基)]三(亚甲基)}三(3-氧杂-2,3-二氢-1H-茚-2,1-二叉)三丙二腈(NFT-C6)和2,2',2″-{[(5,5,10,10,15,15-癸基-10,15-二氢-5H-二茚[1,2-a：1',2'-c]芴-2,7,12-三基)三(噻吩-5,2-二基)]三(亚甲基)}三(3-氧杂-2,3-二氢-1H-茚-2,1-二叉)三丙二腈(NFT-C10). NFT-C6和NFT-C10的最高占据轨道(HOMO)和最低未占轨道(LUMO)分别位于-5.66和-3.75 eV. 其薄膜在400~700 nm范围内具有较大的吸收强度, 最大吸收峰分别位于606和586 nm. 以聚[(2,6-{4,8-二[5-(2-乙基己基)噻吩-2-基]-苯并[1,2-b：4,5-b']二噻吩})-{5,5-(1',3'-二-2-噻吩基-5',7'-二(2-乙基己基)苯并[1',2'-c：4',5'-c']二噻吩-4,8-二酮)}](PBDB-T)为给体材料, 以NFT-C6或NFT-C10为受体材料制备了太阳能电池器件, 器件在300~700 nm之间具有较宽的响应光谱, 其光电转换效率(PCE)分别达到1.09%和5.23%. 原子力显微镜(AFM)结果表明, PBDB-T和NFT-C10共混制备的光伏器件活性层具有合适的相分离尺寸, 有利于激子的有效解离, 而PBDB-T: NFT-C6器件的活性层相分离尺寸过大, 增加了激子复合的几率, 使器件的短路电流、 填充因子和PCE降低. 研究结果表明, 基于三聚茚的星型光伏材料具有一定的应用前景.     

Synthesis and Characterization of Two‐Photon Chromophores Based on a Tetrasubstituted Tetraethynylethylene Scaffold

A new series of model dye molecules composed of three multibranched analogues based on the tetrasubstituted tetraethynylethylene structural motif have been synthesized and experimentally shown to possess strong and widely dispersed two‐photon absorption (2PA) in the near‐IR region. It was found that the spectral position of the major 2PA band could be tuned by the electronic nature of the selected substitution units. The studied model fluorophores also exhibited fairly low photodegradation of their fluorescence intensity even under prolonged UV‐light irradiation, which is beneficial for the development of fluorescence probes that are needed for long‐term light exposure. Furthermore, representative chromophores were selected to demonstrate the power‐control properties within the femtosecond and nanosecond time domains.     

高疲劳寿命氯丁橡胶基减振材料的结构与性能

以氯丁橡胶(CR)为基体材料, 将新型反式-1,4-丁二烯-异戊二烯共聚橡胶(TBIR)引入传统CR减振基体中, 探讨TBIR在减振材料中的应用前景. 研究发现, 随着TBIR用量的增加, CR/TBIR混炼胶的强度及模量明显提升; CR/TBIR硫化胶的拉伸强度、 撕裂强度、 压缩永久变形、 动静刚度比及耐疲劳性能均得到改善, 特别是一级疲劳寿命提高了50%~400%(未填充体系)及40%~180%(填充体系), 六级疲劳寿命提高了60%~500%(未填充体系)及30%~120%(填充体系). 与未填充CR/TBIR硫化胶相比, 填充CR/TBIR硫化胶由于炭黑补强作用及填料-聚合物相互作用的引入, 屈挠疲劳寿命、 撕裂强度及拉伸性能均显著提高. 与填充CR硫化胶相比, 填充CR/TBIR质量比为90/10的并用胶能够在保持硫化胶的损耗因子基本不变的基础上, 实现综合性能的平衡提升.     

Synthesis and Characterization of Two‐Photon Active Chromophores Based on Tetrathienoacene (TTA) and Dithienothiophene (DTT)

Three new donor–π–donor (D‐π‐D) tetrathienoacene (thieno[2′,3′:4,5]thieno[3,2‐b]thieno[2,3‐d]thiophene (TTA))‐cored chromophores, end‐functionalized with electron‐donating triphenylamine (TPA) groups, were developed and characterized for their two‐photon‐related properties by using both nano‐ and femtosecond laser pulses as the probing tools. TTA‐based chromophores exhibit stronger and more widely dispersed two‐photon absorption (2PA) than those of dithienothiophene (DTT)‐based congeners. As a consequence, the bithiophene‐conjugated TTA chromophore exhibits the highest maximum 2PA cross‐section value (up to 2500 GM) with good thermal stability, and thus, it is the best performing two‐photon chromophore among the studied model compounds. The bithiophene‐conjugated DTT analogue exhibits the second highest maximum two‐photon absorptivity of 1950 GM, which is nearly 7 times larger than that of previously reported DTT‐based chromophores.     

Synthesis and self‐organization properties of copolyurethanes based on perylenediimide and naphthalenediimide units

A series of perylene and naphthalene diimide‐containing random copolyurethanes with different ratios of perylene/naphthalene diimide content was synthesized and characterized. Copolymerization improved the solubility of these rigid aromatic diimides, and the copolymers were soluble in common organic solvents like chloroform, tetrahydrofuran, and so forth. The absorption spectra of perylene‐based copolymers showed a red‐shifted peak at a wavelength of 557 nm corresponding to J‐type aggregates. For naphthalene copolymers, the quenching of fluorescence at higher naphthalene incorporation suggested the presence of aggregates because of the extensive π‐π stacking of the aromatic core. FTIR spectroscopic analysis showed that the hydrogen bonding tendency of the polymer decreased with increase in perylene/naphthalene incorporation. The fluorescence spectra of the perylene polymers were exactly a mirror image of the absorption spectra. The fluorescence spectra of the naphthalene polymers at higher naphthalene incorporation showed a red‐shifted excimer like emission peak, which was assigned as static excimers based on their excitation spectra. These polymers could exhibit two types of secondary interaction modes, namely, hydrogen bonding (via urethane linkage) and π‐stacking (via aromatic perylene or naphthalene units) thus highlighting the importance of polymer design in inducing self‐organization at both low and high incorporation of the rigid bisimide moieties. © 2009 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 47: 1224–1235, 2009     

Insensitive and Thermostable Energetic Materials Based on 3‐Ureido‐4‐tetrazole‐furazan: Synthesis,Characterization, and Properties

Energetic salts composed of ureido, furazan, and tetrazole were prepared by simple and efficient chemical routes to explore new insensitive and thermostable energetic materials. 3‐Ureido‐4‐tetrazole‐furazan ( 3 ) and its ammonium salt ( 5 ) and hydrazinium salt ( 6 ) were confirmed by single‐crystal X‐ray diffraction. The thermal stabilities of the synthesized salts were studied using differential scanning calorimetry, and the detonation performances of these salts were calculated using EXPLO 5 V6.01. All the salts exhibit good thermal stability (Td: 148–259 °C) and mechanical sensitivities (IS > 40 J, FS > 360 N), and their detonation velocities range from 7316 to 8655 m · s^–1. Compounds 6 and 10 are potential candidates as novel insensitive and heat‐resistant explosives because of their high detonation temperatures of 247 and 256 °C, good detonation velocities of 8432 and 8523 m · s^–1, and good detonation pressures of 25.6 and 26.8 GPa.     

N-甲基吡咯烷酮与HnXMo12O40·mH2O(X=P,Si,Ge)电荷转移盐的合成、表征及非线性光学性质

由 N-甲基吡咯烷酮 (NMP)和 Hn XMo1 2 O40 · m H2 O(X=P,Si,Ge)合成了具有非线性光学性质的电荷转移盐 ,(NMPH ) 3PMo1 2 O40 · CH3CN ( ) ,(NMPH) 4Si Mo1 2 O40 · CH3CN ( )和(NMPH) 4Ge Mo1 2 O40 · CH3CN( ) ,并以元素分析 ,红外光谱 ,漫反射电子光谱进行了表征 .结果表明 ,杂多酸形成电荷转移盐后其阴离子结构未变 ;N-甲基吡咯烷酮通过 N原子与酸中的质子H 结合成阳离子而成盐 ,在高压汞灯照射下阴阳离子之间可以发生电荷转变 .非线性光学性质研究表明 ,电荷转移盐的倍频效应强度分别为 I2ω =0 .3IKDP,I2ω =0和 I2ω =0 .0 2 IKDP,三阶非线性系数分别为χ( 3) =5 .0× 10 - 1 4 esu,χ( 3) =3.1× 10 - 1 3esu和χ( 3) =4.3× 10 - 1 3es     

Tetranuclear Zn(II) Complex Based on an Asymmetrical Salamo‐Type Chelating Ligand: Synthesis,Structural Characterization,and Fluorescence Property

A new tetranuclear Zn(II ) complex, [{Zn(L)(μ‐OAc )Zn(H₂O )}₂], based on an asymmetrical salamo‐type bisoxime chelating ligand H₃L (6‐hydroxy‐4′‐chloro‐2,2′‐[ethylenediyldioxybis(nitrilomethylidyne)]diphenol) was synthesized and characterized by elemental analyses, differential thermal methods, single‐crystal X‐ray crystallography, and IR , UV –vis, and fluorescence spectra. The Zn(II ) complex crystallizes in the triclinic system, space group P ‐1 with cell parameters a = 9.0742(6) Å, b = 11.8225(5) Å, c = 12.4182(8) Å, Z = 2, V = 1212.56(12) ų , R ₁ = 0.0572, and wR ₂ = 0.1734. The environment of the tetranuclear Zn(II) complex is penta‐coordinated having a slightly distorted trigonal bipyramidal geometry. Moreover, a 1D chain supramolecular structure is formed along the c ‐axis by the intermolecular C1–H1B⋯O14 hydrogen bonds; in the same manner, C2–H2C⋯Cg2 functions in the formation of supramolecular structures along the a ‐axis of the 1D chain. A 2D supramolecular structure along the ac plane extends infinitely under the force of intermolecular hydrogen bonds. Differential scanning calorimetry‐thermogravimetry thermal analysis provides evidence of the coordination of Zn(II) atoms to the ligand H₃L. The Zn(II) complex shows intense photoluminescence with a maximum emission at ~453 nm upon excitation at 360 nm.