侧链含分散红类染料基团的聚(氨酯-酰亚胺)的合成与表征

采用两步法合成了4种侧链含偶氮染料发色团分散红-19的新型聚(氨酯-酰亚胺)(PUI):先合成含染料发色团的二异氰酸酯,再进一步和二酐单体缩合生成PUI.用红外光谱、紫外-可见光谱、DSC和TGA等手段对合成的PUI进行表征.所有PUI在～490nm处都有一强吸收峰.PUI可溶于强极性非质子溶剂,如NMP,DMAc,DMF,DMSO和1,4-丁内酯,有些甚至在常用的低沸点溶剂如THF中也可溶解.PUI的特性粘数在0.16～0.31dL/g范围内.其玻璃化转变温度(Tg)在171～211℃范围内,明显高于侧链型非线性光学聚氨酯(PU).以刚性相对较大的六氟异丙叉基二(3,4-邻苯二甲酸酐)(6FDA)和甲苯-2,4-二异氰酸酯(TDI)为单体的PUI具有比以二苯醚-3,3′,4,4′-四甲酸二酐(OPDA)和4,4′-二异氰酸酯二苯甲烷(MDI)为单体的PUI更高的T_g.PUI的TGA曲线上有两个明显的失重台阶,起始热分解温度大约在300℃左右.     

纳米增强聚(氨酯-酰亚胺)泡沫的研究

聚(氨酯-酰亚胺)(PUI)泡沫是一种兼具聚氨酯和聚酰亚胺优异性能的新型泡沫材料,而纳米增强方法是其增强改性的一种有效手段,这就使纳米增强PUI泡沫成为其纳米复合材料的一个重要发展方向。本文介绍了纳米增强PUI泡沫的研究概况,重点综述了纳米二氧化硅(纳米SiO2)/PUI、多面体低聚倍半硅氧烷(POSS)/PUI、碳纳米管/PUI、蒙脱土/PUI体系的复合泡沫研究进展,着重讨论了纳米SiO2/PUI和POSS/PUI复合泡沫的制备技术,并评述了碳纳米管/PUI复合泡沫、蒙脱土/PUI复合泡沫的主要进展。     

两种高聚物生物芯片材料的光学透过及激光加工性能分析

用准分子激光对高聚物材料进行微加工制作,可以获得比较理想的高聚物基生物芯片.根据对制作生物芯片材料的性能要求,比较了聚甲基丙烯酸甲酯(PMMA)和聚碳酸酯(PC)对不同波长激光的光波透过率,测量了高聚物材料经准分子激光微加工后的微结构,并得出准分子激光对不同髙聚物材料的刻蚀速率与入射激光能量密度之间的关系.     

NCO自由基与SO_2、CS_2反应的速率常数

利用波长为266nm的激光光解CHBr3产生CH自由基,其与NO反应作为NCO自由基的来源.在298K,总压2660Pa的条件下,采用激光诱导荧光的方法,研究了NCO自由基与SO2、CS2的反应.得到了NCO自由基与SO2、CS2双分子反应速率常数分别为(1.8±0.3)×10-11和(3.1±0.4)×10-12cm3·molecule-1·s-1.对这两个反应在B3LYP/6-31 G(d)的水平上进行理论研究的结果表明,NCO自由基与SO2、CS2的反应是加成反应,其机理是NCO自由基中的N原子攻击反应物的中心原子,得到加成产物.     

不同取代基的噻碳菁和吲哚碳菁染料对其在溴化银微晶上吸附能力及形成J-聚集体尺寸分布的影响

本文研究了5-位不同取代基的噻碳菁和吲哚碳菁染料对其在立方型颗粒和T-颗粒溴化银微晶上吸附能力的影响,并采用ACFEM(Analytical Color Fluore scence Electron Microscopy)研究了上述结构染料对其吸附在溴化银微晶所形成的J-聚集体尺寸分布的影响。实验结果表明,对吲哚碳菁染料来说,立方体溴化银微晶表面的吸附能力较T-颗粒溴化银微晶表面的吸附能力强;但对噻碳菁染料来说则相反,它们在T-颗粒溴化银微晶表面的吸附能力较立方体溴化银微晶表面的吸附能力强。另外,对5-位不同取代基的噻碳菁染料而言,无论是在立方型颗粒或T-颗粒溴化银微晶上的吸附能力来说,含取代基(无论4-取代基是吸电子型还是推电子型)的噻碳菁染料较未取代的噻碳菁染料强;而5-位取代基是吸电子型的噻碳菁染料更有利于其吸附在T-颗粒溴化银微晶表面。此外,本文还进一步证明了溴化银微晶表面上染料J-聚集体的生长过程是符合奥斯瓦尔特成熟过程的。吲哚碳菁染料在T-颗粒溴化银微晶上形成的J-聚集体的平均尺寸明显大于在立方体溴化银微晶上形成的J-聚集体的平均尺寸。吸附在立方体溴化银微晶上的5-不同取代基的噻碳菁染料对其形成J-聚集体尺寸分布的影响的研究结果表明,含取代基(-CH₃,-Ph,-Cl)的噻碳菁染料形成的J-聚集体的尺寸分布几乎相同,但与未取代的噻碳菁染料形成的J-聚集体的尺寸分布明显不同;5-位含取代基的噻碳菁染料形成的J-聚集体平均尺寸大于未取代的噻碳菁染料的。     

氩离子激光固化环氧树脂制作三维微结构

利用激光束进行三维成像是通过逐层光引发聚合形成宏观尺度的三维实体 .最近出现的激光全息光刻技术是利用激光束的干涉产生三维全息图案 ,让感光树脂在全息图案中曝光 ,从而一次形成三维周期有序微结构 .通过调节激光干涉及波长可控制三维结构的形状及尺寸 .利用该技术获得亚微米尺度上周期性重复的三维微结构 ,可用于制作三维光子晶体 [1,2 ]等具有独特性能的聚合物材料 .本文用铁芳烃化合物与特种环氧树脂配制成阳离子型可见光固化树脂 ,在氩离子激光器产生的多束可见连续激光相干形成的空间干涉光场中曝光 ,成功地制备出亚微米量级的三…     

激光光散射和电子自旋共振技术研究十二烷基硫酸钠与聚乙烯吡咯烷酮的相互作用

应用动态激光光散射(DLS)和电子自旋共振(ESR)测定研究了单长链表面活性剂十二烷基硫酸钠(SDS)与聚乙烯吡咯烷酮(PVP)相互作用.DLS测定结果表明:SDS在水中形成动力学半径约为61 nm的胶束聚集体,PVP在水中卷曲成动力学半径约为12 nm的线圈,DLS确定的SDS临界胶束浓度(cmc)为6.4×10^-3 mol·L^-1, PVP-SDS具有强的相互作用,PVP分子缠绕在SDS胶束聚集体的周围,屏蔽了SDS胶束聚集体表面碳氢基团与连续水相的接触;ESR结果表明:自由基探针5-doxyl stearic acid在SDS形成胶束聚集体后,从一个较强极性的连续相转变到较小极性的胶束聚集体内核中,胶束聚集体内核的微粘度较纯水的大,SDS与PVP复合聚集体的微观粘度较SDS胶束溶液的大,ESR确定SDS的cmc为6.8×10^-3 mol·L^-1.     

一系列阳离子性卟啉化合物的基质辅助激光解吸质谱行为

应用基质辅助激光解吸电离飞行时间质谱(MALDI-TOF-MS)研究了一系列阳离子性卟啉化合物的质谱行为.结果表明,阳离子性卟啉与非离子性卟啉化合物的激光解吸电离方式有明显不同.对于四-氮R基(R=甲基,乙基,丙基,苄基)吡啶基卟啉,吡啶基氮上的侧链基团(R)可明显影响该类化合物在MALDI-TOF-MS测试过程中离子形成方式;R基团的增大以及平衡阴离子半径的增大可增加平衡阴离子与卟啉环阳离子之间相互作用力的共价成分,因此在MALDI-TOF-MS测定过程中能够得到卟啉环阳离子与多个平衡阴离子结合在一起的较高质量数的离子峰.另外,还初步探讨了阳离子性卟啉化合物的激光解吸电离机理.     

单晶硅表面周期性微结构的减反射特性及光伏特性

利用聚苯乙烯胶体球自组装技术和纳米压印技术在单晶硅表面构筑了两种周期性微结构. 反射光谱表明, 两种周期性微结构都能够对特定波长的入射光有一定的减反射效果; 表面光电压谱和吸收光谱相对应, 在具有减反射效果的波长范围内观察到了表面光电压增强的现象, 说明这种表面构筑微结构的技术可以有效地利用在单晶硅太阳能电池的制造和设计上, 从而提高单晶硅太阳能电池的光电转换效率. 对这种周期性微结构的减反射机理进行了初步探讨.     

牛血清蛋白在共聚物水凝胶接触镜材料上的沉积过程研究

将水凝胶膜样品置于牛血清蛋白(BSA)的水溶液中,沉积一定时间后,采用染料染色结合分光光度法分析沉积前后BSA浓度的变化,计算沉积量,并采用洗脱法测试BSA与水凝胶材料的结合程度.结果表明,BSA的沉积过程为不可逆过程;BSA的沉积作用不受共聚物水凝胶材料中NVP(N-乙烯基吡咯烷酮)结构单元吸附作用的控制;BSA与水凝胶材料松散结合,很容易洗脱;沉积在水凝胶膜表面上的BSA对后续沉积过程无影响.     

钒氧酞菁薄膜瞬态光电压性能的研究

本文分别用1064nm, 532nm和 355nm激发波长的YAG脉冲激光对所制备的phase Ⅱ结构钒氧酞菁膜Al\phase ⅡVOPc\ITO夹心电池进行瞬态光电压响应研究.随着3种波长激发光脉冲强度的增加, 瞬态光电压信号均增强. 激发光波长1064nm、532nm处于酞菁膜Q-带吸收区肩部, 光电压的极性与激发光入射方向无关, 均为负信号; 而激发光波长 355nm处于酞菁膜B-带, 光电压的极性与激发光入射方向有关, 从ITO极方向激发产生正电压信号, 从A1极激发产生负电压信号. 激发光波长对夹心电池的光电压产生有明显的作用, 光电压产生过程中应存在不同的机理. 这与前文^[1]对同一夹心电池稳态光电压响应研究所推断的结论一致.     

Photoresponding ionic complex containing azobenzene chromophore for use in birefringent flm简

A novel photoresponding ionic complex （PANDAZO） was prepared by the ionic self-assembly （1SA） of sodium polyacrylate （PANa） and azobenzene chromophores （NDAZO）. The ionic complex forms an interdigitated lamellar structure with full overlap of the side chains. The optical anisotropy was investigated by using a polarization pulse laser （355 nm）. Furthermore, a high photoinduced birefringence （An = 0.365） was measured by using a continuous 488 nm laser as the pump light.     

Laser‐induced periodic surface structure on a polymer surface: The effect of a prerubbing treatment on the surface structure

The influence of the mechanical rubbing of a polyimide (PI) film on the laser‐induced periodic structure (LIPS) was demonstrated. The periodicity and amplitude of LIPS were greater when the rubbing direction was parallel to the laser polarization direction. The amplitude became small and the periodicity of LIPS did not show an obvious change when the rubbing direction was perpendicular to the laser polarization direction. The effect of the rubbing pretreatment on LIPS was explained on the basis of the wave‐guide effect of rubbing‐induced microgrooves on LIPS formation. The orientation of PI chains induced by mechanical rubbing was relaxed after laser irradiation, and a new orientation of PI chains was formed during the LIPS formation. When the rubbing direction was perpendicular to the laser polarization direction, the orientation of PI chains remained in the rubbing direction. The laser‐irradiated, perpendicularly rubbed PI surface could be used to verify the effects of surface morphologies and intermolecular interactions on liquid‐crystal alignment. © 2003 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 41: 1273–1280, 2003     

Fast and stable recording of birefringence and holographic gratings in an azo-polymethacrylate using a single nanosecond light pulse

Pulsed light-induced recording in azobenzene polymers has recently been studied due to its potential use in optical storage applications. In this paper we study the photoinduced birefringence (Deltan) and holographic grating recording in an azobenzene side chain liquid-crystalline polymethacrylate irradiating with a single 4 ns light pulse at 532 nm. For some irradiation conditions, Deltan grows in less than 50 ns reaching an essentially stable value of about 10(-2). Holographic gratings have been registered using intensity and polarization patterns. Fast response and stability, similar to those of Deltan, was observed in the holographic recording process. Both light-induced anisotropy and relief contributions have been found in the case of gratings recorded using intensity patterns, relief being the dominant contribution at high recording energies. Polarization gratings have been recorded using two orthogonally circularly polarized beams. The resultant gratings showed stable efficiencies up to 0.8% (measured at 633 nm in 1-mum-thick films) and no measurable relief was observed.     

Voltage-pulsed and laser-pulsed atom probe tomography of a multiphase high-strength low-carbon steel

The differences in artifacts associated with voltage-pulsed and laser-pulsed (wavelength = 532 or 355 nm) atom-probe tomographic (APT) analyses of nanoscale precipitation in a high-strength low-carbon steel are assessed using a local-electrode atom-probe tomograph. It is found that the interfacial width of nanoscale Cu precipitates increases with increasing specimen apex temperatures induced by higher laser pulse energies (0.6-2 nJ pulse(-1) at a wavelength of 532 nm). This effect is probably due to surface diffusion of Cu atoms. Increasing the specimen apex temperature by using pulse energies up to 2 nJ pulse(-1) at a wavelength of 532 nm is also found to increase the severity of the local magnification effect for nanoscale M2C metal carbide precipitates, which is indicated by a decrease of the local atomic density inside the carbides from 68 ± 6 nm(-3) (voltage pulsing) to as small as 3.5 ± 0.8 nm(-3). Methods are proposed to solve these problems based on comparisons with the results obtained from voltage-pulsed APT experiments. Essentially, application of the Cu precipitate compositions and local atomic density of M2C metal carbide precipitates measured by voltage-pulsed APT to 532 or 355 nm wavelength laser-pulsed data permits correct quantification of precipitation.     

Enhanced photochemical‐shift of reflection band from an inverse opal film based on larger birefringent polymer liquid crystals: Effect of tolane group on the photochemical shift behavior

Photo‐chemically tunable photonic band gap materials are prepared by infiltration of liquid crystal polymers having azobenzene groups into voids of SiO₂ inverse opal films. Linearly polarized (LP) light irradiation results in transformation from a random to an anisotropic molecular orientation of azobenzene side chains in the voids of the SiO₂ inverse opal film, leading to the reversible and stable shift of the reflection peak to longer wavelength more than 15 nm. To improve switching properties, we use copolymers of azobenzene monomer and tolane monomer, which have higher birefringence, as infiltration materials into the voids. The azobenzene‐tolane copolymers are found to show higher birefringence than azobenzene homopolymers by the LP light irradiation at higher temperature. Consequently, the reflection band of the SiO₂ inverse opal film infiltrated with the azobenzene‐tolane copolymer can be shifted to longer wavelength region more than 55 nm by the irradiation of LP light. © 2009 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 47: 1981–1990, 2009     

Study of Linear and Nonlinear Optical Properties of Four Derivatives of Substituted Aryl Hydrazones of 1,8‐Naphthalimide

Four 1,8‐naphthalimide hydrazone molecules with different electron‐donating groups have been applied in the study of linear and nonlinear optical (NLO) properties. These compounds showed strong green emission in solution. Their NLO properties such as two‐photon absorption (TPA) behavior with femtosecond laser pulses ca. 800 nm and excited‐state absorption (ESA) behavior with nanosecond laser pulses at 532 nm were investigated. Compound 4 presented the largest two‐photon cross section (550 GM) among them due to two factors: the conjugated length of compound 4 is the longest and the electron‐donating ability of compound 4 is the strongest. Different from TPA behavior, compound 2 showed the best nonlinear absorption properties at 532 nm and its nonlinear absorption coefficient and third‐order nonlinear optical susceptibilities χ ⁽³⁾ were up to 1.41×10^?10 MKS and 4.65×10^?12 esu, respectively. Through the modification of the structure, the nonlinear optical properties of these compounds at different wavelengths (532 and 800 nm) were well tuned. The great broad‐band nonlinear optical properties indicate hydrazones are good candidates for organic nonlinear optical absorption materials.     

酞菁锂薄膜的光电流极性研究

利用旋转涂膜法和真空镀膜法制备了以酞菁锂薄膜为工作层的有机光电器件, 结构为氧化铟锡/聚二氧乙基噻吩: 聚对苯乙烯磺酸/酞菁锂/聚偏氟乙稀/铝(ITO/PEDOT: PSS/LiPc/PVDF/Al). 在可见光和近红外脉冲激光照射下, 研究了器件的光电流极性. 在532 nm脉冲激光照射下, 器件的外电路光电流方向从ITO流向铝; 但在1064 nm脉冲激光照射下, 其外电路光电流极性发生反向, 即从铝流向ITO. 酞菁锂薄膜的吸收光谱和X射线衍射谱图显示, 其对可见和近红外光有非常广的吸收, 且为x晶型. 酞菁锂自由基的双极性特性可随入射光波长的变化而改变.     

Generation of surface energy patterns by single pulse laser interference on self-assembled monolayers

Single pulse laser interference lithography is used to structure self-assembled monolayers of thiols on gold. This structuring process is investigated by attenuated total reflection measurements, and a demixing process of a binary polymer blend is used to visualize the produced surface energy pattern. The lithography can be realized with different wavelengths (266, 532, and 1064 nm) which shows that the structuring is a thermal process. As a first demonstration of this process, structures down to 800 nm period and 300 nm width are fabricated.