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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Parameters Affecting Electron Injection Dynamics from Ruthenium Dyes to Titanium Dioxide Nanocrystalline Thin Film
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Parameters Affecting Electron Injection Dynamics from Ruthenium Dyes to Titanium Dioxide Nanocrystalline Thin Film

机译:影响钌染料向二氧化钛纳米晶薄膜电子注入动力学的参数

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摘要

Electron injection rates from Ru(dcbpy)_2(X)_2 [X = 2NCS, 2CN, and dcbpy: dcbpy = 2,2'-bipyridine-4,4'-carboxylate] (called Ru535 or Ru N3, Ru505, and Ru470) to TiO_2 nanocrystalline thin films are examined as a function of adsorbate redox potential, pH of the solution, excitation wavelength, and solvent. For all three dyes, the injection kinetics are biphasic, consisting of a distinct ultrafast component (<100 fs) and slower components. Under different experimental conditions, the partitioning between these two components and the rate of the slow components change, but the rate of the fast component shows no noticeable variations within the ~200 fs time resolution of the measurement. When Ru535, Ru505, and Ru470 were compared at the same pH, increasing amplitude and decreasing rate of slow component were observed, correlating with less negative excited-state redox potentials in these dyes. An analogous trend was seen for RuN3/TiO_2 by increasing the pH of the solution from pH = 2 to 8 and changing from pH = 2 aqueous solution to a (1:1) ethylene/propylene carbonate mixture. The injection dynamics are also dependent on excitation wavelength. The relative amplitude of the slow component increases when the excitation wavelength is changed from 400 to 630 nm. All data can be described by a two-state injection model, which attributes the fast (<100 fs) component to injection from a nonthermalized excited state and the slow component to injection from the thermalized excited state. The partitioning between these two components and the rate of the slow components depend on the relative energetics between dye excited states and the conduction band edge.
机译:Ru(dcbpy)_2(X)_2的电子注入速率[X = 2NCS,2CN和dcbpy:dcbpy = 2,2'-联吡啶-4,4'-羧酸盐](称为Ru535或Ru N3,Ru505和Ru470 )对TiO_2纳米晶体薄膜进行了检测,该薄膜是被吸附物的氧化还原电势,溶液的pH值,激发波长和溶剂的函数。对于所有三种染料,注射动力学都是双相的,由独特的超快组分(<100 fs)和慢组分组成。在不同的实验条件下,这两种成分之间的分配以及慢速成分的速率都会发生变化,但是快速成分的速率在测量的约200 fs时间分辨率内没有显示出明显的变化。当在相同的pH下比较Ru535,Ru505和Ru470时,观察到慢速组分的幅度增加和降低速率,这与这些染料的负激发态氧化还原电势较小相关。对于RuN3 / TiO_2,通过将溶液的pH从pH = 2增加到8,然后从pH = 2水溶液变为(1:1)乙烯/碳酸亚丙酯混合物,可以看到类似的趋势。注入动力学也取决于激发波长。当激发波长从400 nm更改为630 nm时,慢速分量的相对幅度增加。所有数据都可以通过两态注入模型来描述,该模型将快速(<100 fs)分量归因于非热激发态的注入,将慢分量归因于热激发态的注入。这两个成分之间的分配以及慢成分的比率取决于染料激发态与导带边缘之间的相对能量。

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