Max Planck Institute for Polymer Research, Ackermannweg 10, D55128, Mainz, Germany.
ACS Nano. 2010 Jul 27;4(7):3909-20. doi: 10.1021/nn1007594.
Layer-by-layer (LbL) deposition of polyelectrolytes within nanopores in terms of the pore size and the ionic strength was experimentally studied. Anodic aluminum oxide (AAO) membranes, which have aligned, cylindrical, nonintersecting pores, were used as a model nanoporous system. Furthermore, the AAO membranes were also employed as planar optical waveguides to enable in situ monitoring of the LbL process within the nanopores by optical waveguide spectroscopy (OWS). Structurally well-defined N,N-disubstituted hydrazine phosphorus-containing dendrimers of the fourth generation, with peripherally charged groups and diameters of approximately 7 nm, were used as the model polyelectrolytes. The pore diameter of the AAO was varied between 30-116 nm and the ionic strength was varied over 3 orders of magnitude. The dependence of the deposited layer thickness on ionic strength within the nanopores is found to be significantly stronger than LbL deposition on a planar surface. Furthermore, deposition within the nanopores can become inhibited even if the pore diameter is much larger than the diameter of the G4-polyelectrolyte, or if the screening length is insignificant relative to the dendrimer diameter at high ionic strengths. Our results will aid in the template preparation of polyelectrolyte multilayer nanotubes, and our experimental approach may be useful for investigating theories regarding the partitioning of nano-objects within nanopores where electrostatic interactions are dominant. Furthermore, we show that the enhanced ionic strength dependence of polyelectrolyte transport within the nanopores can be used to selectively deposit a LbL multilayer atop a nanoporous substrate.
在纳米孔中,根据孔径和离子强度,通过层层(LbL)沉积聚电解质。使用具有排列整齐、圆柱形、不相交的孔的阳极氧化铝(AAO)膜作为模型纳米多孔系统。此外,AAO 膜还被用作平面光波导,以通过光波导光谱学(OWS)在纳米孔内原位监测 LbL 过程。使用具有外围带电基团和直径约为 7nm 的第四代结构定义良好的 N,N-二取代肼磷树枝状大分子作为模型聚电解质。AAO 的孔径在 30-116nm 之间变化,离子强度在 3 个数量级上变化。发现纳米孔内沉积层厚度对离子强度的依赖性明显强于平面表面上的 LbL 沉积。此外,即使孔径远大于 G4-聚电解质的直径,或者在高离子强度下相对于树突状大分子直径,屏蔽长度不重要,纳米孔内的沉积也可能受到抑制。我们的结果将有助于聚电解质多层纳米管的模板制备,并且我们的实验方法可能有助于研究关于静电相互作用占主导地位的纳米物体在纳米孔内分配的理论。此外,我们表明,纳米孔内聚电解质传输的增强离子强度依赖性可用于选择性地在纳米多孔衬底上沉积 LbL 多层。