非线性光学活性的侧链型聚丙二酸酯液晶的合成和性质

通过熔融缩聚法合成了含非线性光学活性硝基偶氮苯液晶基元的聚丙二酸酯侧链液晶聚合物 ,采用FTIR、NMR对其结构进行了表征 ,DSC确定其液晶转变温度 ,并用变温WAXD及偏光显微镜 (POM )研究其液晶性质 ,该聚合物为近晶型液晶聚合物 ,POM观察到典型焦锥织构 ,近晶相WAXD有对应层间距为2 74nm和 1 35nm的两个衍射峰 .聚合物旋涂膜经电晕极化 ,紫外光谱测试求得其取向序参数 =0 33 .     

极化方法对PZT-4压电陶瓷性能的影响

Pb(Zr_1-xTi_x)O₃ (PZT)由于具有优异的综合性能而成为应用最广泛的压电陶瓷。之前研究工作证明了与直流极化(DCP)和交流极化(ACP)相比,采用交流极化和直流极化相结合的方法能进一步提高弛豫铁电单晶材料的压电性能。本工作报道了直流极化、交流极化和交流极化+直流极化后PZT-4压电陶瓷的介电性能和压电性能,探究了直流极化、交流极化和交流极化+直流极化的最佳极化条件。在最佳交流极化+直流极化条件下, PZT-4 压电陶瓷的压电常数(d₃₃)为350 pC/N,相比直流极化(305 pC/N)、交流极化(320 pC/N)分别提高了15%和9%。交流极化后的PZT-4陶瓷样品的应变值(0.08%)高于进行直流极化样品的(应变值0.05%),表明交流极化可以有效提高PZT-4陶瓷的应变值,但是交流极化后应变曲线的滞后增大不利于器件应用,交流极化对硬性压电陶瓷的影响还需要进一步探讨。     

含偶氮分子的ormocer固体薄膜制备及二阶光学非线性

利用溶胶－凝胶（sol-gel)低温合成非晶态技术,以γ－氨基丙基三乙氧基硅烷（3-aminopropyl triethoxysilane,KH550)与γ－缩水甘油醚基丙基三甲氧基硅烷（3－glycidoxy-propltrimethoxysilane,KH560)为先驱体,把Disperse Orange3(DO3)偶氮分子以3wt%的浓度掺杂到上述溶胶与ormocer(organic modified ceramic)体系中,在ITO片上制备成厚度为4μm的DO3／90KH560－10KH550薄膜。经高温电晕极化后,用二次谐波发生装置,测量出薄膜材料的二次谐波强度,并计算出经极化后薄膜材料的p→p的二阶有效极化系数deff=0.11pm/V。极化24小时后,其SHG强度基本保持不变,大约为刚极化后的80％大小,我们认为这主要是由于介质中KH550的引入,其中－NH2基团与DO3中的－NH2之间形成了氢键的作用,以及由氢键引起的介质材料进一步致密化作用,使得DO3分子不易发生弛豫作用,而保持极化后的分子状态。     

分散橙25掺杂的聚合物PMMA薄膜全光极化的研究

制备了以分散橙25为客体的掺杂型有机聚合物PMMA薄膜样品，对之进行了全光极化研究，极化使薄膜产生诱导二阶非线性光学效应，种子光的强度越大，其二阶非线性极化率达到的饱和值越大;种子光的位相差、相对强度比、光场强度等因素影响薄膜的二阶非线性的优劣.     

Computer screen photo-excited surface plasmon resonance imaging

Angle and spectra resolved surface plasmon resonance (SPR) images of gold and silver thin films with protein deposits is demonstrated using a regular computer screen as light source and a web camera as detector. The screen provides multiple-angle illumination, p-polarized light and controlled spectral radiances to excite surface plasmons in a Kretchmann configuration. A model of the SPR reflectances incorporating the particularities of the source and detector explain the observed signals and the generation of distinctive SPR landscapes is demonstrated. The sensitivity and resolution of the method, determined in air and solution, are 0.145 nm pixel⁻¹, 0.523 nm, 5.13 × 10⁻³ RIU degree⁻¹ and 6.014 × 10⁻⁴ RIU, respectively, encouraging results at this proof of concept stage and considering the ubiquity of the instrumentation.     

极化条件对偶氮化合物薄膜中分子取向的影响

 为探索不同的极化条件对分子取向的影响,用旋涂法制备了偶氮主客体掺杂薄膜,并用电晕极化的方法分别在不同温度和厚度条件下使分子取向,通过测量极化前后紫外-可见吸收谱,研究了平均取向因子的变化,并和二次谐波产生结果进行了比较。实验结果表明：对于厚度相同的偶氮薄膜,随着温度的升高,平均取向因子增大,但二次谐波信号强度先增大后减小;温度越接近聚合物玻璃转变温度,分子越容易取向,但温度过高,聚甲基丙烯酸甲酯变为粘滞态,部分偶氮分子容易在高温下蒸发掉,导致二次谐波信号强度降低,而平均取向因子增大;随着薄膜厚度的增大,针-板电极电场造成薄膜内部电场分布的不均匀性增加,极化效率降低,平均取向因子不断减小,二次谐波信号强度先增大后减小。     

Second harmonic generation of thermally poled ZnCl2 or ZnBr2-B2O3-TeO2 glasses and its mechanism

Second harmonic generation (SHG) was observed from halide, in specific, chlorine or bromine-containing tellurite glasses. The magnitude of SHG increased with increasing halides concentration and poling time. Although the mechanism of SHG is still controversial, it is generally accepted that the idea of the deficiency of cations near the anode side cause SHG. However, in the preset oxyhalide glass system without any singly positive charge cation, the polishing of the anode side showed no effect on SHG. On the other hand, the polishing of the cathode side significantly decreased the magnitude of SHG in the present alkali-free oxyhalide glasses. Therefore, the SHG mechanism in the present oxyhalide glass systems is made evident in which the movement of anions results in an anion-deficient layer near the cathode side.     

偶氮聚合物薄膜的吸收谱和二次谐波产生的温度特性

研究了一种偶氮聚合物薄膜的光谱和二阶非线性光学特性.研究结果表明,聚合体中的偶氮发色团以反式异构体形式存在.加热可使分子之间的相互作用减弱,聚集体的聚集程度降低;温度低于70℃时聚集体的结构不会发生变化,分子间相互作用的改变能够完全恢复;高于70℃降温后聚集体聚集程度的降低不能完全恢复.在一定温度下极化可使发色团偶极子定向有序排列,形成J-聚集体.偶氮聚合物薄膜的二阶非线性光学特性起源于偶极子模型,极化温度是影响极化膜二次谐波强度的重要因素之一,该偶氮聚合物薄膜的最佳极化温度约为90℃.     

压电材料裂纹顶端条状电饱和区模型的力学分析

在线性压电本构方程框架下,对裂纹顶端条状电饱和区模型进行了严格的数学分析．完整地考虑了各向异性力电耦合效应．建立了电饱和区尺寸与外加电场的依赖关系．证实了当裂纹垂直极化轴时,压电材料的断裂应力随着外加正电场的增加而减小,随着外加负电场的增加而增加．当裂纹平行于极化轴时,与极化轴平行的外加电场对断裂应力无影响     

STUDY ON THE POLING PROPERTIES OF NONLINEAR OPTICAL ACTIVE DERIVATIVE OF POLY (p-HYDROXYSTYRENE):(PS)O-DCV

In this paper, the poling properties of (PS)O-DCV, a derivative of poly (p-hydroxystyrene ), was reported. The investigations showed that the thermochromism correction, which was neglected in the literatures, should be considered in the measurements of order parameter of poled films with electrochromism technique Here, another linear optical method, IR and polarized IR spectra for characterizing of poled films was suggested first time. The bulk second nonlinear optical coefficient d_(33) of poled films could be estimated by measured order parameter semi-qualitatively.