规则结构钛酸盐自组装聚集体的制备

在水热条件下, 采用不同的钛源, 通过控制溶液碱度和冷却温度等反应条件, 利用无模板自组装技术, 在钛酸盐薄膜表面及溶液相中制备了鸟巢状和绒球状钛酸盐纳米带自组装聚集体以及海胆状钛酸盐纳米管自组装聚集体. 通过引入碳酸钠模板, 制备出形貌新颖的钛酸钠-碳酸钠香蒲状自组装聚集体复合材料. 初步研究了纳米自组装聚集体的形成机理, 认为其形成经历了一维纳米结构(纳米带或纳米管)的生长和一维纳米结构的自组装2个过程.     

双组分偶氮聚合物胶体球制备及其光致形变行为研究

研究了2种环氧树脂类含4-氨基-4′-硝基偶氮苯和4-氨基-4′-羧基偶氮苯生色团聚合物(BP-AZ-NT、BP-AZ-CA)双组分胶体球的制备和光致形变行为.通过在上述聚合物的四氢呋喃溶液中逐步加水诱导自组装的方法,得到了BP-AZ-CA/BP-AZ-NT双组分胶体球.在上述两种聚合物自组装形成胶体球过程中,较为疏水的BP-AZ-NT分子先发生聚集,而较亲水的BP-AZ-CA则在形成的胶体颗粒表面发生进一步聚集.在胶体球形成过程中,体系的临界水含量(CWC)主要由BP-AZ-NT发生聚集时的水含量决定,双组分胶体球的外层则含较多的BP-AZ-CA分子.比较单组分胶体球与双组分胶体球在线偏振Ar+激光(488nm,100mW/cm2)照射下的形变行为,进一步证实了通过上述方法可以制备BP-AZ-CA和BP-AZ-NT双组份的胶体球;胶体球形变时的初始拉伸速率由胶体球的外层聚合物分子的性质所决定。     

聚乙二醇-接枝-聚(γ-苄基L-谷氨酸酯)刚-柔接枝共聚物的合成及其自组装行为研究

通过负离子开环聚合,合成了以柔性亲水的聚乙二醇(PEG)为主链,刚性疏水的聚(γ-苄基L-谷氨酸酯)(PBLG)为侧链的PEG-g-PBLG刚-柔接枝共聚物.运用核磁共振氢谱(1H-NMR)、傅里叶变换红外光谱(FTIR)和凝胶渗透色谱(GPC)等表征了共聚物的结构、分子量及其分布.以共溶剂溶解、选择性溶剂透析的方法制备了自组装聚集体.利用扫描电子显微镜(SEM)、透射电子显微镜(TEM)、原子力显微镜(AFM)和激光光散射(LLS)等表征了共聚物自组装体的形貌和结构.研究发现,基于其特殊的拓扑结构,接枝共聚物的自组装行为表现出与一般规律不同的变化趋势.具有较短疏水PBLG侧链的PEG-g-PBLG可以自组装形成球形复合胶束,随着疏水PBLG侧链的增长,聚集体逐渐由复合胶束转变为囊泡,这种现象在已有的研究中鲜有报道.此外,降低初始聚合物溶液的浓度,共聚物自组装得到的聚集体的尺寸变小而分布变宽;反之,聚集体的尺寸增大而分布变窄.还利用耗散粒子动力学方法,验证了实验中聚集体的形貌变化,并给出了聚集体中的链段分布等在实验中较难得到的信息.     

自组装光致形变功能偶氮分子玻璃微球

通过逐滴滴加去离子水的方法, 探究了具有快速光响应的偶氮分子玻璃(IAC-4)在初始浓度范围为1.0~5.0 mg/mL条件下的自组装, 制备了形貌规整、 尺寸均一的胶体球, 并利用动态光散射技术(DLS)测定了IAC-4胶体球的流体力学半径. 通过测定一系列初始浓度的IAC-4溶液的临界水含量, 探究了IAC-4在自组装过程中析出、 聚集成核和核生长的规律. 研究发现, 临界水含量与IAC-4初始浓度的关系符合二元混合溶剂中固体溶质的溶解度变化规律. 通过调节去离子水的滴加量, 研究了自组装过程中, IAC-4聚集体流体力学半径呈现先增大后减小的趋势. IAC-4胶体球的水分散液, 通过室温干燥得到的固态IAC-4微球在线性偏振激光(488 nm, 100 mW/cm²)垂直辐照下表现出快速的光响应特性. 当辐照时间为1 min时, IAC-4微球快速地拉伸形变, 形成平均长径比为1.44的椭圆形粒子. 随着光辐照时间延长, 平均长径比持续增大. 当辐照时间为7 min时, IAC-4微球被拉伸为棒状粒子, 其平均长径比可高达3.32.     

新型支化侧链偶氮聚电解质的合成与性能研究

通过后重氮偶合的方法合成了一种含支化侧链偶氮苯生色团的聚电解质 (PBANT AC) .用IR、NMR、DSC、UV和元素分析等手段对聚合物的结构和性能进行了表征 .研究发现 ,在不同比例的水和四氢呋喃混合溶剂中PBANT AC的紫外 可见光光谱有很大的差别 .这种差别反映了PBANT AC分子中的偶氮苯生色团的不同聚集状态 .通过静电吸附逐层自组装的方法将PBANT AC分子组装成多层膜 .在 488nm的偏振Ar+ 激光的照射下 ,聚合物薄膜中的偶氮苯生色团可发生光致取向 ,取向有序度约 0 0 5 .偶氮苯生色团的顺反异构化反应使H 聚集体在光照后发生解聚集     

支化侧链偶氮无规共聚物中空和类囊泡聚集体研究

研究了支化侧链型偶氮无规共聚物(PMAPB6P-AA)在THF/H2O混合溶液中的自组装行为.研究发现,通过缓慢增加体系的水含量,可以制备出具有中空结构的非球形聚集体.调节聚合物的初始浓度,可以得到不同粒径的聚集体.聚集体中偶氮生色团的光致异构化速率与异构化程度随聚合物初始浓度的增大而减小.在此基础上,采用更加缓慢的增加水含量的方法,使聚合物分子进行充分的疏水聚集与H-聚集,制备出类囊泡状聚集体.在紫外光照射条件下,观察到类囊泡聚集体发生了光致解聚集.     

超声和光双重调控的AB_2主客体型两亲分子的超分子自组装与程序化控释研究

合成了一种同时含有单偶氮苯基团和双β-环糊精单元的AB2型两亲分子(Azo-CD2),并通过核磁共振谱和基质辅助激光解吸电离飞行时间质谱对其结构进行了表征和确认.动态光散射和透射电子显微镜测试结果表明,在水溶液中,Azo-CD2在无任何外界刺激的条件下可自发地形成球形自组装体,而当施加超声振动后逐渐转变为超分子超支化聚合物自组装体;该自组装体被进一步施加紫外光辐射后可解离成尺寸较小的支化聚集体,而其在可见光辐射下又可以可逆地变回原来的超支化自组装形貌.利用紫外分光光度计测试Azo-CD2自组装体对抗癌药物阿霉素(DOX)的释放曲线发现,通过超声和光的双重调控作用可实现Azo-CD2自组装体对DOX的程序化控制释放.利用一维1H-NMR谱和二维NOESY谱进一步阐明了Azo-CD2自组装体形貌转变过程与其程序化控释结果的相关关系.     

两亲性共轭高分子聚(对亚苯基丁二炔)的合成与二维自组装

设计、合成了两亲性线型共轭聚合物聚(对亚苯基丁二炔)(A-PPB),研究了它在溶液中的二维自组装行为.首先合成了A-PPB的前驱体聚合物PPB,利用核磁氢谱(1H-NMR)、傅里叶红外光谱(FTIR)和拉曼光谱对聚合物的结构及分子量进行了表征.然后通过水解反应,获得了两亲性共轭聚合物A-PPB,并考察了它在水、甲醇以及甲醇/甲苯混合溶剂中的自组装行为.透射电子显微镜(TEM)的测试结果表明,A-PPB在水溶液中自组装形成了二维超分子纳米片(2D-SNS),尺寸达几微米;用原子力显微镜(AFM)测得2D-SNS的厚度为5 nm左右,由不超过3层的二维超分子聚合物层堆积而成.高分辨透射电子显微镜(HRTEM)、选区电子衍射(SAED)及X-射线衍射(XRD)的测试结果表明,2D-SNS是由A-PPB分子链平行堆积而成.在甲醇溶剂中,A-PPB形成了无规聚集体,而在甲醇/甲苯混合溶剂中则自组装形成了多层堆积的二维超分子纳米片.对比研究表明,非亲水的PPB在氯仿/甲醇混合溶剂中形成的是较厚的层状聚集体.还发现聚合物的链长对于自组装形成二维超分子片层也会有影响,当用数均聚合度为8的两亲性低聚(对亚苯基丁二炔)(A-OPB)在水溶液中进行自组装时,只能形成尺寸较小的无规聚集体.由此可见,聚合物的两亲性、电荷排斥作用以及聚合物链长等因素都会对共轭聚合物的二维自组装行为产生重要影响.     

梳状-线性共聚物自组装的耗散粒子动力学模拟

梳状-线性共聚物在选择性溶剂中可以自组装形成两种不同类型的聚集体, 其中第I类的自组装发生在亲、疏溶剂链之间, 而第II类发生在线性链和梳状亚结构之间. 本工作利用耗散粒子动力学方法, 分别研究了梳状-线性共聚物在侧链和主链选择性溶剂中形成的这两类聚集体, 探讨了侧链长度和侧链数量等对聚集体类型及形貌的影响. 研究表明, 第II类聚集体在侧链长度较短且侧链数量较多时容易形成. 将模拟结果与文献报道的实验结果相比较, 发现两者能较好地吻合. 此外, 本研究获得了一些在实验中较难得到的信息, 有助于进一步理解梳状-线性共聚物的自组装行为.     

荧光淬灭法研究疏水缔合共聚物(PAM-b-PPOEA)_n自组装聚集数

运用荧光淬灭技术,包括稳态荧光淬灭法(SSFQ)和时间分辨荧光淬灭法(TRFQ),研究了疏水缔合水溶性丙烯酰胺2苯氧基丙烯酸酯多嵌段共聚物[P(AM POEA)]在水溶液中自组装的聚集数.这类聚合物在水溶液中易形成胶束状聚集体,探针芘分子和淬灭剂二苯酮增溶于疏水微区,荧光测定结果很好地符合Poisson淬灭模型.实验结果表明聚合物链结构、聚合物浓度和无机盐对聚集体的尺寸具有重要影响.聚合物自组装聚集数NA随疏水单体含量的增加和疏水嵌段长度的减小而增大,同时也随聚合物浓度和NaCl浓度增加而增大.另外对聚合物链结构、聚集数和溶液粘度的相互关系进行了讨论.     

Azo polymer colloidal spheres containing different amounts of functional groups and their photoinduced deformation behavior

In this work, colloidal spheres composed of azo polymers with different chromophore loading densities were prepared, and their photoinduced deformation behavior was studied. The colloids were constructed by using a series of amphiphilic epoxy-based random copolymers containing 4-carboxylazobenzene functional groups with different degrees of functionalization (DFs). The colloidal spheres were fabricated through gradual hydrophobic aggregation of the polymeric chains in tetrahydrofuran-H2O dispersion media, which was induced by gradually adding water into the systems. The colloidal spheres were characterized by using transmission electron microscopy and dynamic light scattering. The photoinduced deformation behavior was studied by irradiating the colloidal spheres with a linearly polarized Ar+ laser beam. Results showed that the critical water content (CWC) for the colloid formation is related to the DF of the polymers, and CWC increases with the increase of DF. The hydrodynamic diameter of the colloidal spheres is also related to the DF of the polymers. When the DF of the polymers increases, the average size of the colloids gradually decreases. The hydrodynamic diameter of the colloidal spheres increases as the water dropping rate decreases. When the dropping rate is below 20 microL/s, the size of the colloidal spheres increases abruptly as the dropping rate further decreases. Upon the linearly polarized Ar+ laser beam irradiation, the colloids composed of polymers with different DFs can all be elongated along the polarization direction of the laser beam. As DF increases, the deformation degree characterized by the axial ratio (l/d) almost linearly increases. These observations can give some insight into the photoinduced deformation mechanism and can be used to construct colloids with different sizes and photoresponsive ability.     

Photoinduced deformation of amphiphilic azo polymer colloidal spheres

Photoinduced shape deformation of colloidal spheres made of an amphiphilic azo polymer has been demonstrated in this work. The polymer contains the donor-and-acceptor-type azobenzene chromophores and can form uniform colloidal spheres by dropwise adding water into its THF solution. When the colloidal spheres obtained were exposed to the interfering p-polarized Ar+ laser beams (150 mW/cm2), the colloidal spheres changed to prolates (i.e., "rugby-balls"), "spindles", and finally "rods", depending on the irradiation times. The elongated direction of the spheres was observed to be the same as the polarization direction of the laser beam. The average major-to-minor ratio of the ellipsoids could be easily adjusted by controlling the irradiation time. The deformation effect observed in this work can offer a new way to prepare nonspherical colloids from colloidal spheres and will shed new light on the correlation between the photodriven shape deformation and photoinduced surface relief gratings for the same type of polymers.     

Stretching effect of linearly polarized Ar+ laser single-beam on azo polymer colloidal spheres

This work shows that a linearly polarized Ar+ laser single-beam irradiation can cause stretching deformation of azo polymer colloidal spheres along the polarization direction of the laser beam. An epoxy-based polymer, containing 4-amino-4'-carboxyazobenzene at each repeat unit, was used to construct the colloidal spheres. The colloidal spheres were prepared by gradual hydrophobic aggregation of the polymeric chains in a THF/H2O dispersion medium, which was induced by a steady increase in the water content. When the obtained colloidal spheres were exposed to the spatially filtered and collimated Ar+ laser beam (488 nm, 150 mW/cm2), the colloids were stretched along the polarization direction of the laser beam. In the testing period (20 min), the colloids were deformed continuously as the irradiation time increased. When 2D close-packed arrays of the colloidal spheres were irradiated by the polarized laser single-beam, the colloidal spheres were all uniformly stretched along the polarization direction of the laser beam. On the contrary, when the arrays were irradiated by the interfering p-polarized laser beams, only the colloidal spheres in the bright regions of the interference pattern were significantly deformed.     

Photoinduced alignment of polymer liquid crystals containing azobenzene moieties in the side group VII. On He-Ne laser beam irradiation

Photoinduced alignment in a polymer liquid crystal prepared from 6-{1-[4-(2-cyano-4-nitrophenylazo)phenyl]piperazino}hexyl acrylate and 4'-[6-(methacryloyloxy)hexyloxy]-4-cyanobiphenyl was investigated for the first time on irradiation with a polarized He-Ne laser beam at 633 nm. The azobenzene moieties as well as the inert cyanobiphenyl mesogenic units were aligned with the molecular long axis perpendicular to the polarization direction of the irradiation light. Alignment induced on short irradiation was reversible, while that induced under prolonged irradiation was irreversible due to the occurrence of crosslinking which might be caused by photoinduced decomposition of the azobenzene moieties during the photoirradiation process.     

Formation of bragg gratings with large angular multiplicity by means of the photoinduced reorientation of azobenzene copolymers

Optically transparent thick films of methacrylate copolymer containing donor-acceptor-type azobenzene and cyanobiphenyl moieties were prepared, and their optical properties were explored in terms of a photoinduced change in molecular alignment and the formation of Bragg gratings with angular and polarization multiplicity. Azobenzene moieties substituted with ethoxy, cyano, and nitro groups were employed, and their photoresponsive behavior was investigated. It was found by polarized UV-vis spectroscopy that the alignment of azobenzene moieties in the films was random in the initial state but became perpendicular to the direction of polarization of the writing beam after irradiation with a linearly polarized beam from an Ar+ laser at 514 nm. The film containing the cyanoazobenzene moieties showed the fastest formation of optical anisotropy due to an efficient change in molecular alignment. When two linearly polarized beams from the Ar+ laser were allowed to interfere in the films with a thickness of 200 microm, the diffraction beam was observed immediately and reached 97% upon photoirradiation at 200 mW/cm2 for 5 min. It was clearly observed that the response time became shorter with an increase in the light intensity of the writing beams, maintaining the high diffraction efficiency. Furthermore, it was clearly seen that the diffraction efficiency strongly depended on the direction of polarization of the reading beam. Holographic multiple data storage in a film was demonstrated, and 55 holograms with angular multiplicity were recorded successfully. In addition, multiple data storage using the polarization and angle selectivity simultaneously was first demonstrated.     

Azo polymer microspherical cap array: soft-lithographic fabrication and photoinduced shape deformation behavior

In this work, azo polymer microspherical cap arrays possessing unique photoprocessible properties have been fabricated through a soft-lithographic contact printing approach. In the process, hexagonal polystyrene (PS) colloidal arrays, obtained by the vertical deposition method, were used as masters. Poly(dimethylsiloxane) (PDMS) stamps with aligned hemisphere air voids on the surfaces were obtained by casting the precursor against the colloidal arrays. By using the stamps and a solution of an epoxy-based azo polymer (BP-AZ-CA) as "ink", the microspherical cap arrays were fabricated by pressing the "inked" surfaces against substrates. Uniform 2D arrays of the submicrometer spherical caps could be obtained on the substrates after peeling off the stamps and drying. The characteristic sizes of the arrays depended on some adjustable features, such as the diameters of PS spheres and concentrations of the "inks" used in the process. After exposure to a linearly polarized Ar+ laser single beam, the spherical caps could be stretched along the polarization direction, and the arrays were consequently transformed into ellipsoidal cap arrays. Upon irradiation of interfering p-polarized Ar+ laser beams, only the spherical caps in the bright fringes were deformed by the light irradiation, which resulted in more complicated surface relief patterns. The observation gives another well-defined example of the photoinduced mass migration in the submicrometer scale. The approach can potentially be applied to fabrication of microlens arrays with different converging rate in two directions.     

侧链型偶氮聚合物液晶在不同波长激发条件下的光致取向

合成了聚甲基丙烯酸 (6 [4 (4 氰基偶氮苯 )苯氧基 ]己酯 ) (Poly(6 [4 (4 cyanophenylazo)phenoxy]hexylmethacrylate) (PM6ABCN) ) ,采用溶液挥发法在玻璃载片上成膜 ,研究了薄膜样品在Tg 温度以下的光致取向 .用波长分别为 36 6、40 0和 436nm的偏振光照射 ,发现PM6ABCN薄膜的光致取向过程不仅依赖于光的强度 ,还依赖所使用的偏振光的波长 .在低于Tg 的温度下 ,用波长为 40 0nm ,功率为 2 0mW cm2 的光照射 10 0s可以使样品的取向达到饱和 ,而用 36 6nm的光导致的取向程度要小于 40 0nm和 436nm的光 ,因为 36 6nm的光会在稳态时产生更多数目的cis异构体