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介孔 TiO(2) 中通过后嫁接 SAMs 控制孔径和表面电荷。

Pore size and surface charge control in mesoporous TiO(2) using post-grafted SAMs.

机构信息

Institute of Chemistry, University of Osnabrück, Barbarastrasse. 7, D-49069 Osnabrück, Germany.

出版信息

Phys Chem Chem Phys. 2010 Feb 21;12(7):1473-82. doi: 10.1039/b921743f. Epub 2010 Jan 5.

DOI:10.1039/b921743f
PMID:20126759
Abstract

Two types of TiO(2) are used as mesoporous scaffolds, one (i) randomly sintered yielding an average pore size of 15-20 nm including bottlenecks of 1-3 nm (s-TiO(2)), the other (ii) prepared by evaporation-induced self-assembly with a pore size of 7-9 nm (t-TiO(2)). The pore walls of these materials were post-grafted with phosphonic acids bearing one or two pyridinium or sulfonate head groups via 6, 10 or 14 methylene groups, in order to tune the free pore diameter and the surface charge over a broad range. The modification was characterized by FTIR spectroscopy. Charge transport through the modified pores was investigated by cyclic voltammetry using Fe(CN)(6), IrCl(6) Ru(NH(3))(6), and (ferrocenylmethyl)trimethylammonium as electroactive tracer ions and La(3+) or naphthalene trisulfonate as non-electroactive species. The Faradaic current through the pores is controlled by the combination of surface charge, tracer ion charge, charge of the non-electroactive ions present, as well as the pore diameter. High currents due to strong preconcentration are observed, e.g. a partitioning coefficient value of 7 x 10(3) for Fe(CN)(6) on a modified electrode making it a candidate for ion-exchange voltammetry. Other phenomena presented are: (i) electrostatic closure of the porous system due to overlapping Debye layers, (ii) charge inversion of the pore walls, and (iii) the mode of charge propagation along the pore walls. Interestingly s-TiO(2) is more effective at building up an electrostatic barrier compared to t-TiO(2), probably because of narrow bottlenecks which interconnect the pores in s-TiO(2) only.

摘要

两种类型的 TiO(2) 被用作介孔支架,一种(i)随机烧结,平均孔径为 15-20nm,包括 1-3nm 的瓶颈(s-TiO(2)),另一种(ii)通过蒸发诱导自组装制备,孔径为 7-9nm(t-TiO(2))。这些材料的孔壁通过 6、10 或 14 个亚甲基接枝上带有一个或两个吡啶鎓或磺酸盐头基的膦酸,以在较宽的范围内调节自由孔径和表面电荷。修饰通过傅里叶变换红外光谱法进行表征。通过使用 Fe(CN)(6)、IrCl(6) Ru(NH(3))(6)和(二茂铁甲基)三甲铵作为电活性示踪离子以及 La(3+)或萘三磺酸作为非电活性物质,通过循环伏安法研究了改性孔中的电荷传输。通过孔的法拉第电流受表面电荷、示踪离子电荷、存在的非电活性离子的电荷以及孔径的组合控制。由于强预浓缩而观察到高电流,例如,在修饰电极上 Fe(CN)(6) 的分配系数值为 7 x 10(3),使其成为离子交换伏安法的候选物。呈现的其他现象是:(i)由于重叠的 Debye 层,多孔系统的静电闭合,(ii)孔壁的电荷反转,和(iii)电荷沿孔壁的传播模式。有趣的是,与 t-TiO(2) 相比,s-TiO(2) 更有效地构建静电障碍,这可能是由于 s-TiO(2) 中只有狭窄的瓶颈将孔互连。

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