一种新的具有给体-受体结构的有机分子的合成及LB膜研究

本工作合成了一种新的具有给体-受体结构的长碳链有机分子, 2, 3-二(十六烷硫基)-5-(4'-硝基苯亚甲基)-1, 4-二硫代-2-环戊烯, 对其单分子膜的成膜性能进行了研究。在适宜条件下制备了单层及多层LB膜。通过电子衍射、X射线衍射、紫外-可见吸收光谱等手段对LB膜的结构进行了表征。实验结果表明, 这种化合物的成膜性能很好。单分子层膜的二次谐波测试表明该发色团分子具有较好的二阶非线性光学性。     

新型LB成膜材料—两亲性侧链取代酞菁锌的合成

本文合成了一种新型的两亲性硬脂酸侧链取代的酞菁化合物。利用LB膜技术制备了致菁化合物与正十六烷混合的单层和多层LB膜,LB膜内酞菁分子大环与基片大体平行,表明该分子具有良好的成膜性能。     

酞菁铜化合物LB膜的制备及结构形态研究

利用LB技术研究了带有4个长碳氢链的酞菁铜化合物(CuC12Pc)的单分子膜及它与十八胺(ODA)、二十酸(AA)的混合LB膜的聚集结构形态. 结果表明这种酞菁铜化合物在气液界面上可以形成比较稳定有序的双层Langmuir膜, 且可以转移质量较好的多层LB膜. 利用原子力显微镜(AFM)研究了酞菁铜分子的聚集体结构, 发现CuC12Pc/AA混合膜表现为网状的聚集结构, 而CuC12Pc/ODA混合膜形成长岛颗粒状聚集, 并结合UV-Vis吸收光谱讨论了酞菁铜分子形成不同聚集结构的原因.     

4-(2-甲氧基乙氧基)-三-4-(2,4-二特戊基苯氧基)酞菁铜的合成及其LB膜特性研究

LB膜的特性在很大程度上决定于成膜分子的结构。铜酞菁衍生物具有大π键电子共轭体系,有明显的光电特性,成膜性好,很适于作LB膜气敏材料。我们在前期工作的基础上,为探明气敏特性与化合物结构间的关系,设计并合成了标题化合物,并对其LB膜的气敏特性进行了研究。     

中心对称双酞菁铥LB膜二次谐波产生特性

利用二次谐波产生(SHG)方法研究了中心对称分子稀土夹心双酞菁铥(TmPc₂) Langmuir-Blodgett (LB)膜二阶非线性光学特性, 测量了二次谐波强度随入射基频光入射角的关系, 并对其二阶非线性产生机制进行了讨论. 实验结果表明, TmPc₂分子LB膜具有较好的二次谐波信号, 二次谐波信号强度的最大值在基频光入射角为45°的地方, 其二阶非线性极化率χ⁽²⁾和分子超极化率β分别为1.152×10^-8和1.905×10^-30 esu. 通过测量样品二次谐波信号的偏振特性, 并与理论分析相比较, 得出其二阶非线性起源于电四极子作用机制.     

新型LB成膜材料-两亲性侧链取代酞菁锌的合成

本文合成了一种新型的两亲性硬脂酸侧链取代的酞菁化合物, 利用LB膜技术制备了酞菁化合物与正十六烷混合的单层和多层LB膜, LB膜内酞菁分子大环与基片大体平行, 表明该分子具有良好的成膜性能。     

5,12-二硫杂-7,14-二氮杂-5,7,12,14-四氢并五苯及其相关化合物二阶非线性光学性质的理论研究

在ZINDO方法基础上,按完全态求和(SOS)公式编制了计算分子二阶非线性光学系数β_ijk、β_u的程序.研究了不同取代基在5,12-二硫杂-7,14-二氮杂-5,7,12,14-四氢并五苯侧环取代衍生物及相关化合物的结构、光谱和二阶非线性光学性质。结果表明:侧环上取代推、拉电于基团对增大二阶光学非线性都有利;分子共平面,共轭作用强,对增大二阶光学非线性有利.     

四（2,4—二叔戊基苯氧基）酞菁铜（Ⅱ）的合成及其LB膜

合成了标题酞菁铜衍生物,并通过元素分析,高压液相色谱,紫外光谱,红外光谱,核磁共振谱,电镜,顺磁共振谱及质谱加以确认。该化合物在稀氯仿溶液和LB膜中各以单,双分子缔合的形式存在。Z型沉积形成的单层LB膜对氨气有很高的灵敏度和选择性。     

一种含稀土半菁的二阶非线性光学材料的研究

LB膜技术作为一种重要手段，可以在分子水平上对材料进行组装．有机化合物作为非线性光学材料，由于具有很大的非线性系数、光学响应速度快及光损伤阈值大等优点而受到人们的重视[1]．对于二阶非线性光学材料而言，其发色团分子的非中。心对称结构是其非线性光学信号叠加的必要条件．LB膜技术以其不同的沉积方式，可有效地控制有机分子的排列和取向，形成非中，心对称结构，成为制备高性能二阶非线性光学材料的良好手段．我们首先将疏水性的稀土配阴离子引入非线性光学成膜材料中，由于其体积较大，可以避免对形成LB膜不利的H聚体的生成…     

气/液界面上双萘菁夹心化合物有序超分子结构的组装

研究了气/液界面上双(八-十二烷硫基)萘菁铒{Er[Nc(SC₁₂H₂₅)₈]₂}形成的Langmuir单层膜中的超分子结构. 表面压-面积(π -A)等温线表明该化合物形成了稳定的单层膜. 将其沉积在云母片上, 用原子力显微镜(AFM)进行观察, 表明分子形成了取向高度有序的结构, 聚集体特征长度在100 nm左右(有的长达300 nm), 宽为20~30 nm.用紫外-可见光谱、偏振紫外-可见光谱、小角X射线衍射等对 LB膜进行了研究, 发现分子大环平面与基片平面夹角为54°, 每层厚度为3.53 nm. 研究表明形成的超分子结构由4~6列以面对面堆积形成的柱状体构成.     

Cd[CH_3O(OH)C_6H_3CH=N(CH_2)_2OH]_2Br_2的合成、结构及微观二阶非线性光学系数

合成了标题配合物Cd[CH3O(OH)C6H3CH =N(CH2 ) 2 OH]2 Br2 ,对其进行了元素分析、红外和X射线结构分析。该配合物单晶的分子式为 :CdC2 0 H2 6N2 O6Br2 ,Mr=662 .66属于单斜晶系 ,P2 1 /n空间群 ,晶胞参数a =7.851 2 (2 ) ,b =1 7.391 (3) ,c=1 7.575(4) ,β =90 .86(3)°,V =2 392 (1 ) 3,Z =4,Dc=1 .834g·cm- 3,μ(MoKα) =4.2 4 1 9mm- 1 ,F(0 0 0 ) =1 30 4。用直接法解得结构 .R =0 .0 74,Rw=0 .0 84.在 2 99± 1K的温度下收集到 3744个独立衍射点 ,其中 2 4 70个为可观察的衍射点 [I≥ 3σ(I) ]。同时在 1 .0 64μm的Nd :YAG激光器上对配合物进行了粉末SHG实验 ,并用MOPAC软件包采用PM 3方法解得其分子的微观二阶极化率为 3.341× 1 0 - 30 esu。进一步讨论了微观二阶非线性极化率、宏观激光倍频效应和分子结构、晶体结构之间的关系。     

芪类分子掺杂极化聚合膜的非线性光学性质

采用实时测量光学二次谐波产生（SHG）和吸收光谱的方法时芪类有机分子DANS（4’－N,N－dimethylamino－nitrostilbene）及一种新合成的经氰基团修饰的有机分子CNDS（α’－cyano－4’－nitro－4－N,N－dimethylaminostilbene）掺杂PMMA[poly（methylmethacrylate）]极化聚合膜的非线性光学性质进行了研究。在电晕极化条件下,由于聚合膜的电导率随温度的变化急剧增加,实验中发现两种掺杂极化聚合膜的最佳电导极化温度均低于它们的玻转温度Tg．在最佳极化条件下,从极化前和极化后的吸收光谱变化可看出CNDS的有序度较DANS的差．但实时SHG表明,CNDS／PMMA极化掺杂聚合膜的二阶非线性系数X（2）较DANS／PMMA极化聚合膜的大．结合极化前和极化后吸收峰强度的变化,我们得到CNDS分了的非线性极化率β约为140×10-30esu.在撤离极化场后,CNDS／PMMA的SHG强度的弛豫也比DANS／PMMA慢,说明CNDS是一种性能较DANS优越的制备二阶光学非线性的掺杂分子．     

Langmuir-Blodgett Film Formation and Optical Second Harmoni Generation of a Hemicyanine Derivative

Langmuir-Blodgett (LB) film of a hemicyanine derivative, (E)-N-hexadecyl-4-[2-(4-dimethylaminophenyl)ethenyl]pyridinium bromide (Hc) was fabricated. The Langmuir film of Hc exhibited good transfer behaviour. Optical second harmonic generation from the LB film was measured. Macroscopic second-order susceptibilily, molecular hyperpolarizability and tilt angle for the molecules on a substrate were estimated to be 7.06×10^-6 esu, 6.47×10^-27 esu,and 31.6° respectively.     

SYNTHESIS AND CHARACTERIZATION OF NOVEL SOL-GEL DOPED ORGANIC／INORGANIC HYBRID NONLINEAR OPTICAL MATERIALS

4-hydroxy-4 ‘-nitro azobenzene (NHA) and 4-amino-4 ‘-nitro azobenzene (DO3) were prepared respectively from p-nitrophenylamine as a precursor compound. Two kinds of doped organic/inorganic hybrid nonlinear optical (NLO) materials containing NHA and DO3 were synthesized by Sol-Gel process. The preparation and properties of two NLO materials were studied and characterized by FTIR, IH-NMR, UV-VIS, SEM, DSC and SHG measurements. The results show that the maximum doping amounts of NHA and DO3 in two doped hybrid NLO materials are 7.2(wt)% and ll.3(wt)% respectively, and the corresponding second-order NLO coefficients (d33values) are 2.91 ×l0^-3esu and 6.14×10 -8 esu. Two doped NLO materials have relatively good RT stability, after 90 days at RT the d33 values can maintain about 85% of their initial values, but after l0h at 100℃ can only maintain about 50% of their initial values. In this report, the reasons for high-temperature instability of doped materials were discussed, and the possible improvements were also suggested.     

两种Ni(Ⅱ)配合物的合成及三阶非线性光学性能

合成了两种新的Ni(Ⅱ)配合物,用UV、IR、MS和元素分析进行了表征。采用飞秒激光,运用简并四波混频法,研究了Ni(Ⅱ)配合物在非共振状态下的三阶非线性光学性能。它们的三阶非线性光学极化率χ(3)为3.21×10-13 esu和3.58×10-13 esu,非线性折射率n2为5.89×10-12 esu和6.58×10-12 esu,分子二阶超极化率γ为3.21×10-31 esu和3.57×10-31 esu,响应时间τ为54 fs和59 fs。探索了配合物的分子结构对三阶非线性光学性能的影响。结果表明具有大的高度离域的π电子共轭体系是获得较大三阶非线性光学性能的关键。     

Study on second harmonic generation of 9-benzylidene-substituted-10-methyl-9,10-dihydroacridines

Eight 9-benzylidene-substituted-10-methyl-9,10-dihydroacridine derivatives were synthesized from acridine as starting material and were characterized by 1H-NMR, 13C-NMR, Ms and elemental analysis. The second harmonic generation (SHG) values of these compounds were determined in powder using Nd:YAG as a laser source, as compared with urea powder, and the values of second-order polarizabilities (betaxxx), the values of the composite magnitude (betaCTmicrog) of molecular hypersusceptibilities and their moment of these compounds were obtained by the solvatochromic method under ground state for everyone. The results showed that SHG value of 10 is higher than that of urea; the betaCTmicrog of 5 (107.8 x 10(-30) esu) is lower than that of 4-nitro-N,N-dimethylaniline (30 x 10(-30) esu); the betaCTmicrog of 7 (350.8 x 10(-30) esu) and 10 (244.6 x 10(-30) esu) are higher than that of 4-nitro-N,N-dimethylaniline; the betaCTmicrog of 8 (3553 x 10(-30) esu), 11 (1187 x 10(-30) esu) and 12 (1163 x 10(-30) esu) are much more higher than that of 4-nitro-N,N-dimethylaniline. The results demonstrated that this series of compounds possesses good second-order nonlinear optical (NLO) property. The regular relationship could not be obtained between electronegativity of substituents (R) attached to benzylidene ring and SHG values or betaCTmicrog values although the Rs are different in electronegativity and should make an effect on the extent of intramolecular electron-transfer and would consequently influence SHG or betaCTmicrog. The electron-withdrawing ability of R from benzylidene ring played an important role on lambdamax of these compounds.     

Growth and characterization of Fe3+-doped bis(thiourea)zinc(II) chloride crystals

Fe3+-doping at ～10 mol% in aqueous medium during crystal growth by slow evaporation solution method in bis(thiourea)zinc(II) chloride (BTZC) leads to form a new compound C2H8Cl2N4S2Zn0.93Fe0.07 (BTZCF) which crystallizes in orthorhombic structure with centrosymmetric space group Pnma though the parent compound BTZC crystallizes in noncentrosymmetric structure with space group Pn2(1)a. The interesting feature observed in this new crystal is that though it crystallizes in centrosymmetric structure, it exhibits positive SHG result (weak signal), quite likely due to possible surface effects or internal stress. The calculated first-order hyperpolarizability is 1.457×10(-30) esu which is ～5.5 times that of urea. Fe3+-doping enhances the transmittance to a significant extent. Comparison of the thermal analysis results by DSC reveals the incorporation of dopant into the crystalline matrix. The high resolution XRD studies reveal that the crystalline quality is improved considerably when the doping level is reached to ～10 mol%.     

Interaction between nitric oxide and lipid-like DDPA LB film investigated with SHG and AFM

Interactions between Nitric oxide (NO) and DDPA Langmuir-Blodgett (LB) film are investigated with second harmonic generation (SHG) and atomic force microscopy (AFM). It has been found that the adsorption of NO molecules on DDPA LB film only changes the value of the second-order susceptibility of the DDPA molecule on film but not its orientation.     

A Novel Amphiphilic Push-pull Ferrocene Derivative: Langmuir-Blodgett Films and Second-order Optical Nonlinearity

We investigated Langmuir-Blodgett(LB) films built from the mixture of an amphiphilic push-pull ferrocene derivative(P) and behenic acid. Langmuir films of P diluted by behenic acid exhibit a very good cohesion, and the mixed films can easily be transferred onto solid substrates. Linear dichroism UV-visible and IR spectroscopy measurements of the mixed LB multilayers confirm that the molecules(P) are oriented to the substrate. The nonlinear optical experiments on the mixed monolayer deposited on the CaF₂ slide showed that P displays efficient optical second harmonic generation(SHG) with a molecular hyperpolarizability (β)h, high as 6.0×10^-29e. s. u..