dos Santos David S, Cardoso Marcos R, Leite Fabio L, Aroca Ricardo F, Mattoso Luiz H C, Oliveira Osvaldo N, Mendonça Cleber R
Materials & Surface Science Group, School of Physical Sciences, University of Windsor, Windsor, ON, Canada N9B 3P4.
Langmuir. 2006 Jul 4;22(14):6177-80. doi: 10.1021/la060399q.
The fabrication of nanostructured layer-by-layer (LbL) films strives for molecular control of the film properties directly connected with modifications in the film architecture. In the present report, the photoinduced birefringence and formation of the surface-relief gratings in LbL films obtained with an azopolymer (PS119) are shown to be strongly affected by the generation of the dendrimer employed in the alternating layers. Stronger adsorption of PS119 occurred when polypropylenimine tetrahexacontaamine dendrimer (DAB) of higher generations is used, due to a larger number of sites available to interact with azochromophores in PS119. In contrast, the photoinduced birefringence for LbL films made with the generation 1 dendrimer (DABG1) was higher, which can be explained by weaker interactions between adjacent layers. Strong interactions in LbL films consisting of PS119 and generation 3 or 5 dendrimers restrict the chromophore mobility, leading to a smaller birefringence. The interpretation is supported by the fact that surface-relief gratings with larger amplitudes were obtained for 35-bilayer films of DABG1/PS119 (31 nm) in comparison with films from DABG5/PS119 (5 nm). These gratings were formed with mass transport arising from a light-driven mechanism, as photoinscription was successful only with p-polarized light and not with s-polarized light.
纳米结构逐层(LbL)薄膜的制备旨在对与薄膜结构变化直接相关的薄膜性质进行分子控制。在本报告中,由偶氮聚合物(PS119)制得的LbL薄膜中的光致双折射和表面浮雕光栅的形成被证明受到交替层中使用的树枝状大分子的强烈影响。当使用更高代数的聚亚丙基亚胺四十二胺树枝状大分子(DAB)时,PS119的吸附更强,这是因为有更多的位点可用于与PS119中的偶氮发色团相互作用。相比之下,由第一代树枝状大分子(DABG1)制成的LbL薄膜的光致双折射更高,这可以用相邻层之间较弱的相互作用来解释。由PS119和第三代或第五代树枝状大分子组成的LbL薄膜中的强相互作用限制了发色团的迁移率,导致双折射较小。这一解释得到了以下事实的支持:与DABG5/PS119薄膜(5nm)相比,DABG1/PS119的35层薄膜(31nm)获得了更大振幅的表面浮雕光栅。这些光栅是由光驱动机制引起的质量传输形成的,因为光写入仅在p偏振光下成功,而在s偏振光下不成功。