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Polymer-grafted gold nanorods in polymer thin films: Dispersion and plasmonic coupling.

机译:聚合物薄膜中的聚合物接枝金纳米棒:分散和等离子体耦合。

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摘要

This dissertation describes complementary experimental and theoretical studies to deter- mine the thermodynamic factors that affect the dispersion of polymer-grafted Au nanorods within polymer thin films. Au nanorods exhibit a uniform dispersion with a regular spacing for favorable brush / matrix interactions, such as poly(ethylene glycol) (PEG)-Au / poly(methyl methacrylate) (PMMA) and polystyrene (PS)-Au / poly(2,6-dimethyl-p-phenylene oxide) (PPO). For PEG-Au / PMMA, the nanorods are locally oriented and their dispersion is independent of the ratio of the degree of polymerization of the matrix (P) to that of the brush (N), α = P/N, whereas for chemically similar brush / matrix combinations, such as PS-Au / PS and PEG-Au / poly(ethylene oxide) (PEO), nanorods are randomly dispersed for α 2. For aggregated systems (α > 2), nanorods are found primarily within aggregates containing side-by-side aligned nanorods with a spacing that scales with N. UV-visible spectroscopy and discrete dipole approximation (DDA) calculations demonstrate that coupling between surface plasmons within the aggregates leads to a blue shift in the optical absorption as α increases, indicating the sensitivity of spectroscopy for determining nanorod dispersion in polymer nanocomposite films. Self-consistent field theory (SCFT) calculations and Monte Carlo (MC) simulations show that the aggregation of nanorods for α > 2 can be attributed to depletion-attraction forces caused by autophobic dewetting of the brush and matrix. Finally, miscible blends of PS and PPO are investigated as a route to control depletion-attraction interactions between PS-Au nanorods. Initially, nanorods aggregate in matrices having 50 vol. % PPO and then gradually disperse as PPO becomes the majority component. The brush and matrix density profiles, determined by SCFT, show that PPO segregates into the PS brush, and acts as a compatibilizer, which improves dispersion. As dispersion improves, coupling between surface plasmons is reduced, leading to a red shift in the optical absorption. The outcome of these systematic structure-property-modeling studies is the ability to control nanorod dispersion, orientation, and optical absorption by manipulating brush/matrix interactions and entropic depletion-attraction forces.
机译:本文描述了互补的实验和理论研究,以确定影响聚合物接枝的金纳米棒在聚合物薄膜中分散的热力学因素。金纳米棒表现出均匀的分散度,并具有规则的间距以实现良好的笔刷/基体相互作用,例如聚(乙二醇)(PEG)-Au /聚(甲基丙烯酸甲酯)(PMMA)和聚苯乙烯(PS)-Au /聚(2, 6-二甲基对苯撑氧)(PPO)。对于PEG-Au / PMMA,纳米棒是局部取向的,其分散度与基质(P)与刷子的聚合度(N)的比率无关,α= P / N,而对于化学相似的刷子/基质组合,例如PS-Au / PS和PEG-Au /聚环氧乙烷(PEO),纳米棒随机分散为α2。对于聚集系统(α> 2),纳米棒主要存在于含有以下物质的聚集体中并排排列的纳米棒,间距与N成比例。紫外可见光谱法和离散偶极近似(DDA)计算表明,聚集体中表面等离激元之间的耦合会导致随着α的增加,光吸收发生蓝移,表明光谱法测定聚合物纳米复合材料薄膜中纳米棒分散度的敏感性。自洽场理论(SCFT)计算和蒙特卡洛(MC)模拟表明,当α> 2时,纳米棒的聚集可归因于刷子和基质的自疏水性润湿引起的耗尽吸引力。最后,研究了PS和PPO的可混溶共混物,以控制PS-Au纳米棒之间的耗尽-吸引相互作用。最初,纳米棒聚集在体积为50 vol。 PPO百分比,然后随着PPO成为主要成分而逐渐分散。由SCFT确定的刷子和基体密度曲线表明,PPO偏析到PS刷子中,并充当增容剂,从而改善了分散性。随着色散的改善,表面等离激元之间的耦合降低,导致光吸收发生红移。这些系统的结构特性模型研究的结果是,通过操纵刷子/基质相互作用和熵损耗力,可以控制纳米棒的分散,取向和光吸收。

著录项

  • 作者

    Hore, Michael-Jon Ainsley.;

  • 作者单位

    University of Pennsylvania.;

  • 授予单位 University of Pennsylvania.;
  • 学科 Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2012
  • 页码 203 p.
  • 总页数 203
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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