Lana-Villarreal T, Bisquert J, Mora-Seró I, Salvador P
Instituto de Catalisis y Petroleoquímica, CSIC, Madrid, Spain, Departament de Ciències Experimentals, Universitat Jaume I, 12080 Castelló, Spain.
J Phys Chem B. 2005 May 26;109(20):10355-61. doi: 10.1021/jp050182p.
Nanostructured TiO(2) thin-film electrodes of controlled thickness were obtained by immobilization of TiO(2) powder (Degussa P25) on SnO(2):F (FTO)-coated glasses by electrophoresis. The photocurrent-potential characteristics of the electrodes in contact with an indifferent aqueous electrolyte, for both front--and backside UV illumination, show the existence of a macroscopic electric field in the electrode region near the FTO substrate. This electric field, which is only photoinduced in the presence of water (it does not appear in TiO(2) dye-sensitized solar cells under visible illumination), apparently disappears when an efficient hole scavenger, like methanol, is added to the aqueous electrolyte. It is attributed to a nonhomogeneous spatial accumulation of photogenerated holes at surface-bound OH radicals resulting from the photooxidation of chemisorbed water molecules. The influence of film thickness and UV illumination mode (front- and backside) on the photoinduced electric field is analyzed by solving the transport equations for diffusion and drift of electrons.
通过电泳将二氧化钛粉末(德固赛P25)固定在涂有二氧化锡:氟(FTO)的玻璃上,获得了厚度可控的纳米结构二氧化钛薄膜电极。对于正面和背面紫外线照射,电极与中性水性电解质接触时的光电流-电势特性表明,在靠近FTO基板的电极区域存在宏观电场。该电场仅在有水的情况下由光诱导产生(在可见光照射下的二氧化钛染料敏化太阳能电池中不存在),当向水性电解质中添加有效的空穴清除剂(如甲醇)时,该电场明显消失。它归因于光氧化化学吸附水分子产生的表面结合羟基自由基上光生空穴的非均匀空间积累。通过求解电子扩散和漂移的输运方程,分析了膜厚度和紫外线照射模式(正面和背面)对光诱导电场的影响。