采用微流注射法在光纤端面制备单层胶体微球薄膜

提出了一种在光纤端面制备单层胶体晶体薄膜的新方法——微流注射法,利用针尖微量注射胶体微球溶液,该方法可以在气/液界面直接形成大面积六角密排的周期纳米球阵列,面积达到平方厘米级别,再利用二维胶体单层膜的可转移性,将薄膜转移至到光纤端面衬底上,形成单层胶体微球有序薄膜.采用扫描电子显微镜和光谱分析仪对样品形貌、结构以及光学特性进行了表征和分析.电子显微镜图像表明,光纤端面的胶体晶体为六角密排阵列结构.透射光谱表明,该结构具有光子晶体的带隙特征,带隙的中心波长约为700和850 nm,与分析软件FDTD Solutions仿真结果相吻合.结合溅射沉积方法,得到了银纳米球壳阵列结构,检验了其局域表面等离子体共振效应(LSPR).对比讨论了溶液浓度、弯月面的形成及注射速度等因素对微流组装胶体微球薄膜质量的影响.     

金属Al薄膜基微池强制沉积胶体光子晶体的制备

强制沉积法是一种利用自组装原理快速沉积胶体晶体有序阵列的模板方法. 我们利用微机械刻划法加工金属Al薄膜, Al膜厚控制微粒粒径和聚醚砜膜厚控制层数, 成功地制备了用于强制沉积光子晶体的微池装置. 为了检验该微池装置的有效性, 我们分别测试了不同粒径(224, 245和283 nm)单分散聚苯乙烯微球的沉积效果, 并且对其中一种微球(283 nm)进行了不同温度的烘干处理, 检验了烘干温度对该样品表面形貌和光子带隙中心波长的影响. 实验结果表明, 该光子晶体呈面心立方结构, 内部晶格完整, 缺陷较少, 带隙中心波长的实验值与计算值符合得较好. 此外, 烘干处理可以使构成光子晶体的微球发生微观变化, 并导致光子带隙中心波长的蓝移.     

金属AI薄膜基微池强制沉积胶体光子晶体的制备

强制沉积法是一种利用自组装原理快速沉积胶体晶体有序阵列的模板方法.我们利用微机械刻划法加工金属Al薄膜,Al膜厚控制微粒粒径和聚醚砜膜厚控制层数,成功地制备了用于强制沉积光子晶体的微池装置.为了检验该微池装置的有效性,我们分别测试了不同粒径(224,245和283 nm)单分散聚苯乙烯微球的沉积效果,并且对其中一种微球(283 nm)进行了不同温度的烘干处理,检验了烘干温度对该样品表面形貌和光子带隙中心波长的影响.实验结果表明,该光子晶体呈面心立方结构,内部晶格完整,缺陷较少,带隙中心波长的实验值与计算值符合得较好.此外,烘干处理可以使构成光子晶体的微球发生微观变化,并导致光子带隙中心波长的蓝移.     

流动控制沉积法制备PMMA叠层光子晶体薄膜及其光学性能研究

采用流动控制沉积法, 通过调控泵速和聚甲基丙烯酸甲酯(PMMA)胶体微球溶液的浓度, 制备出微球排列高度有序且薄膜紧密附着于基底的高质量光子晶体薄膜. 获得了制备高质量PMMA光子晶体薄膜的组装条件范围, 发现在该条件范围内, 当泵速或胶体微球溶液浓度一定时, PMMA光子晶体薄膜的厚度随胶体微球溶液浓度的增加或泵速的降低而增加. 研究了组装条件对PMMA光子晶体薄膜光学性能的影响, 发现光子禁带位置随光子晶体薄膜厚度增加或减少而红移或蓝移. 在此基础上, 控制组装条件得到了不同尺寸微球堆叠而成的叠层光子晶体薄膜, 并研究了其光学性能的变化规律. 结果显示, 叠层光子晶体薄膜的光子禁带峰为各层叠层光子晶体禁带峰的简单叠加, 且峰强度受光入射角方向影响.     

TiO2掺杂调控聚苯乙烯微球折射率及胶体光子晶体结构色

胶体光子晶体由于其可调变的结构色在绿色印刷、印染等领域备受关注,而其光子带隙的宽度和位置由光子晶体的晶格参数(晶面间距,通常受胶体微球尺寸影响)和介质的折射率决定。现有人工胶体光子晶体主要基于SiO_2和高分子(如聚苯乙烯(PS)等)微球的组装制备,由于胶体微球材质种类有限,折射率调控受限,因而目前调控胶体光子晶体结构色主要靠改变胶体微球的尺寸来实现。本文首先制备高折射率(2.6)的TiO_2纳米晶,在乳液聚合制备单分散的PS(折射率1.6)微球过程中,将所制备的TiO_2纳米晶掺杂于PS微球中,通过TiO_2的掺杂量有效调控胶体微球的折射率,进而实现胶体光子晶体的结构色调控。以多色胶体光子晶体微球的水溶液为墨水,采用彩色喷墨打印技术打印了电脑设计的光子晶体彩画。本文发展的光子晶体结构色调控新技术拓展了胶体光子晶体的应用。     

改性聚苯乙烯微球的制备及其胶体晶体的组装

采用甲基丙烯酸改性的无皂乳液聚合方法制备了尺寸为210 nm、含羧基的聚苯乙烯(PS)微球，用红外光谱、透射电子显微镜和粒度分析仪对其形状和结构进行分析，结果表明，经甲基丙烯酸改性后得到了表面为高密度电荷的单分散性PS微球.用垂直沉积法快速制备出在较大范围(大于1 cm2)呈现很好有序性的密排结构聚苯乙烯胶体晶体薄膜，其在590 nm波长处存在光子带隙.在电子显微镜下，观察到这种胶体晶体是面心立方(fcc)密排结构.     

带隙可调各向同性蛋白石光子晶体的制备与研究

用旋涂法将聚苯乙烯微球组装成光子晶体,研究了此光子晶体的特点,并分析了在单一微球粒径下旋涂参数对光子带隙的影响.结果表明:旋涂法制备的光子晶体具有各向同性特点,其光子带隙由旋涂参数决定.光子晶体的反射波段取决于乳液中微球的质量分数,而反射强度取决于旋涂层数.因此,在设计光子晶体时,可以根据需要,通过微球的质量分数和旋涂...     

P(HEMA-co-AM)胶体晶体膜的制备及其性能

将聚苯乙烯胶体晶体嵌入丙烯酰胺(AM)与甲基丙烯酸羟乙酯(HEMA)的交联共聚膜中,制备了共聚物P(AM-co-HEMA)胶体晶体膜.研究了单体配比及交联剂N,N'-亚甲基双(丙烯酰胺)(MBA)对胶体晶体膜的光子带隙峰位置、拉伸强度和断裂伸长率的影响.结果表明:当n(HEMA)/n(AM)≤2.33时,光子带隙峰较明...     

基于胆甾相液晶的可调制光子晶体

将胆甾相液晶填充进胶体晶体内部空隙, 通过胆甾相液晶与胶体晶体的耦合, 构建了一种新型可调制液晶光子晶体. 填充于胶体晶体内部的胆甾相液晶织构呈现典型的手性近晶相(S)特征. 由于胆甾相液晶具有特定的选择性反射, 当胶体晶体的带隙处于胆甾相液晶的反射波长范围之内, 则随着温度的改变, 胶体晶体的带隙与胆甾相液晶的带隙同时发生蓝移. 在一定温度条件下, 胆甾相液晶的带隙将与胶体晶体的带隙发生耦合, 实现了光子晶体带隙在单峰与双峰之间的可逆切换.     

胶体自组装法形成光子带隙材料*

光子带隙晶体使人们可以有效地控制和操纵光子,但是构建光子晶体,尤其是近红外及可见光区域的光子晶体是一个困难的工作,它对材料提出了很高的要求.本文从化学的角度,利用自组装方法,对胶体晶体和反蛋白石等类光子带隙材料包括半导体、金属、金属氧化物、聚合物、染料等进行较全面的介绍,同时介绍了如何从这些材料获得光子带隙.     

基于生物素-亲和素相互作用的胶体晶体阵列的构筑与特性

将胶体晶体阵列(crystalline colloidal arrays,CCA)的Bragg衍射特性与水凝胶的刺激响应性功能结合起来,可制成一种有效的对特定分子具有识别和响应能力的传感材料.采用无皂乳液聚合制备的单分散聚(苯乙烯-4-苯乙烯磺酸钠)纳米颗粒,通过表面电荷的静电斥力可自组装形成CCA,经光聚合固定在水凝胶网络内形成聚合胶体晶阵(polymerized CCA).在水凝胶网络中用共价结合引入生物素分子,通过强的亲和相互作用可与蛋白质亲和素生成生物素-亲和素复合物,在水凝胶网络中形成交联点,引起水凝胶体积相变,进而导致CCA晶面间距发生改变,从而引发Bragg衍射波长发生相应的移动.     

Polymerized PolyHEMA photonic crystals: pH and ethanol sensor materials

The surface of monodisperse silica particles synthesized using the Stober process were coated with a thin layer of polystyrene. Surface charge groups were attached by a grafting polymerization of styrene sulfonate. The resulting highly charged monodisperse silica particles self-assemble into crystalline colloidal arrays (CCA) in deionized water. We polymerized hydroxyethyl methacrylate (HEMA) around the CCA to form a HEMA-polymerized crystalline colloidal array (PCCA). Hydrofluoric acid was utilized to etch out the silica particles to produce a three-dimensional periodic array of voids in the HEMA PCCA. The diffraction from the embedded CCA sensitively monitors the concentration of ethanol in water because the HEMA PCCA shows a large volume dependence on ethanol due to a decreased Flory-Huggins mixing parameter. Between pure water and 40% ethanol the diffraction shifts across the entire visible spectral region. We accurately modeled the dependence of the diffraction wavelength on ethanol concentration using Flory theory. We also fabricated a PCCA (which responds to pH changes in both low and high ionic strength solutions) by utilizing a second polymerization to incorporate carboxyl groups into the HEMA PCCA. We were also able to model the pH dependence of diffraction of the HEMA PCCA by using Flory theory. An unusual feature of the pH response is a hysteresis in response to titration to higher and lower pH. This hysteresis results from the formation of a Donnan potential at high pH which shifts the ionic equilibrium. The kinetics of equilibration is very slow due to the ultralow diffusion constant of protons in the carboxylated PCCA as predicted earlier by the Tanaka group.     

重金属离子敏感型聚合物胶体晶体的研究

以含有双硫键的二丙烯酰胱胺与双丙烯酰胺作为交联剂, 与单体丙烯酰胺紫外光引发聚合, 嵌入聚苯乙烯胶体晶体, 制备了聚丙烯酰胺胶体晶体水凝胶. 将水凝胶中双硫键打断形成巯基, 利用巯基可与重金属离子偶合的作用, 水凝胶体积收缩而改变胶体晶体中胶粒之间的距离, 根据胶体晶体带隙位移, 可分析水中重金属离子的浓度. 紫外可见光反射图谱表明, 胶体晶体带隙最大可蓝移约80 nm. 带隙移动与时间的关系曲线表明, 胶体晶体水凝胶对重金属离子有较好的灵敏度. 该体系可用于分析铅、锌等重金属离子.     

Photonic crystal carbohydrate sensors: low ionic strength sugar sensing

We developed a carbohydrate sensing material, which consists of a crystalline colloidal array (CCA) incorporated into a polyacrylamide hydrogel (PCCA) with pendent boronic acid groups. The embedded CCA diffracts visible light, and the PCCA diffraction wavelength reports on the hydrogel volume. This boronic acid PCCA responds to species containing vicinal cis diols such as carbohydrates. This PCCA photonic crystal sensing material responds to glucose in low ionic strength aqueous solutions by swelling and red shifting its diffraction as the glucose concentration increases. The hydrogel swelling results from a Donnan potential due to formation of boronate anion; the boronic acid pK(a) decreases upon glucose binding. This sensing material responds to glucose and other sugars at <50 microM concentrations in low ionic strength solutions.     

Modeling of stimulated hydrogel volume changes in photonic crystal Pb2+ sensing materials

We modeled the stimulated hydrogel volume transitions of a material which binds Pb2+ and is used as a photonic crystal chemical sensing material. This material consists of a polymerized crystalline colloidal array (PCCA) hydrogel which contains a crown ether molecular recognition group. The PCCA is a polyacrylamide hydrogel which embeds a crystalline colloidal array (CCA) of monodisperse polystyrene spheres of approximately 100 nm. The array spacing is set to diffract light in the visible spectral region. Changes in the hydrogel volume induced by Pb2+ binding alter the array spacing and shift the diffracted wavelength. This system allows us to sensitively follow the hydrogel swelling behavior which results from the immobilization of the Pb2+ by the crown ether chelating groups. Binding of the Pb2+ immobilizes its counterions. This results in a Donnan potential, which results in an osmotic pressure which swells the hydrogel. We continue here our development of a predictive model for hydrogel swelling based on Flory's theory of gel swelling. We are qualitatively able to model the PCCA swelling but cannot correctly model the large responsivity observed at the lowest Pb2+ concentrations which give rise to the experimentally observed low detection limits for Pb2+. These PCCA materials enable stimulated hydrogel volume transitions to be studied.     

Development of a new sensor material based on crystalline colloidal arrays embedded into polymer network

This study reports the development of a novel sensing material that reports on analyte concentrations via diffraction of visible light from polymerized crystalline colloidal arrays (PCCA). The PCCA contains periodic crystalline colloidal array (CCA) of spherical polystyrene colloids. This new method permanently locks the order of the CCA by embedding the CCA into a polymer network. These materials are mostly used in the development of novel materials which are basically called sensors for metal ions and all kinds of organic molecules. The polymer around the crystalline colloid can be functionalized with some recognition molecule, making these materials useful as optical sensors. We developed a sensor, utilizing crown ether, 2-aminomethyl-18-crown-6 (2A18C6) as the recognition agent, that detects K⁺ in the concentration range from 5 to 160 ppm.     

Non-affine structural evolution of soft colloidal crystalline latex films under stretching as observed via synchrotron X-ray scattering

A polymer dispersion consisting of soft latex spheres with a diameter of 135 nm was used to produce a crystalline film with face-centered cubic (fcc) packing of the spheres. Different from conventional small-molecule and hard-sphere colloidal crystals, the crystalline latex film in the present case is soft (i.e., easily deformable). The structural evolution of this soft colloidal latex film under stretching was investigated by in-situ synchrotron ultra-small-angle X-ray scattering. The film exhibits polycrystalline scattering behavior corresponding to fcc structure. Stretching results not only in a large deformation of the crystallographic structure but also in considerable nonaffine deformation at high draw ratios. The unexpected nonaffine deformation was attributed to slippage between rows of particles and crystalline grain boundaries. The crystalline structure remains intact even at high deformation, suggesting that directional anisotropic colloidal crystallites can be easily produced.     

Structural characterization of thin hydroxypropylcellulose films. X-ray reflectivity studies

Thin solid films of hydroxypropylcellulose (HPC) have been investigated using synchrotron X-ray reflectivity. Evidence of preferential alignment of HPC molecules at the substrate surface is obtained. In the surface region the liquid crystalline domains ofHPC are preferentially oriented parallel to the substrate, whereas in the bulk they are mostly distributed randomly. Incorporation of colloidal particles in the film-substrate region destroys the preferential alignment. It is also found that in conditions of restricted geometry (very thin films), a minimum film thickness is required to produce lateral packing order perpendicular to the substrate surface.     

Thin film interference of colloidal thin films

A stairlike colloidal crystal thin film composed of poly(styrene-methyl methacrylate-acrylic acid) (P(St-MMA-AA)) monodispersed colloids was fabricated on an inclined silicon substrate. Different bright colors were observed on the various parts of the film with different layers as white light irradiated perpendicularly on it. The relationship between the colors and layers of the film was investigated and discussed according to the principle of thin film interference. On the basis of the phenomenon of thin film interference, a one-layer colloidal film having uniform color was researched and it would display diverse colors before and after swollen by styrene (St). A circular stairlike colloidal film was achieved to mimic the colors of the peacock tail feather.     

Inverse opal photonic crystal of chalcogenide glass by solution processing

Chalcogenide opal and inverse opal photonic crystals were successfully fabricated by low-cost and low-temperature solution-based process, which is well developed in polymer films processing. Highly ordered silica colloidal crystal films were successfully infilled with nano-colloidal solution of the high refractive index As(30)S(70) chalcogenide glass by using spin-coating method. The silica/As-S opal film was etched in HF acid to dissolve the silica opal template and fabricate the inverse opal As-S photonic crystal. Both, the infilled silica/As-S opal film (Δn ~ 0.84 near λ=770 nm) and the inverse opal As-S photonic structure (Δn ~ 1.26 near λ=660 nm) had significantly enhanced reflectivity values and wider photonic bandgaps in comparison with the silica opal film template (Δn ~ 0.434 near λ=600 nm). The key aspects of opal film preparation by spin-coating of nano-colloidal chalcogenide glass solution are discussed. The solution fabricated "inorganic polymer" opal and the inverse opal structures exceed photonic properties of silica or any organic polymer opal film. The fabricated photonic structures are proposed for designing novel flexible colloidal crystal laser devices, photonic waveguides and chemical sensors.