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首页> 外文期刊>The Journal of Chemical Physics >ULTRAFAST STUDY OF INTERFACIAL ELECTRON TRANSFER BETWEEN 9-ANTHRACENE-CARBOXYLATE AND TIO2 SEMICONDUCTOR PARTICLES
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ULTRAFAST STUDY OF INTERFACIAL ELECTRON TRANSFER BETWEEN 9-ANTHRACENE-CARBOXYLATE AND TIO2 SEMICONDUCTOR PARTICLES

机译:9-蒽型羧酸盐和TiO2半导体颗粒之间界面电子转移的超快研究

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The excited state dynamics of 9-anthracene-carboxylic acid adsorbed onto the surface of TiO2 semiconductor particles were examined with ca. 250 fs time resolution. A combination of transient absorption and time-resolved anisotropy measurements show that approximately 76% of the photo-excited dye molecules transfer an electron to the TiO2 particles. The time scale for the forward electron transfer reaction was determined to be less than or equal to 1 ps. The 9-anthracene-carboxylate radical cations produced by this reaction undergo back electron transfer on a 54 ps time scale. A more accurate estimate of the forward electron transfer reaction time is not possible, due to the contribution to the transient absorption signal from adsorbed dye molecules that do not transfer electrons to TiO2. These nonreactive species are deactivated by either nonradiative decay or fluorescence emission. The fluorescence spectrum from the dye molecules bound to the TiO2 particles is very different to that of the free dye in solution. The free dye has a broad red-shifted spectrum, whereas, the adsorbed molecules have a structured spectrum that displays a small Stokes shift. The red shift in the free dye fluorescence spectrum is due to stabilization of the excited electronic state through torsional motion of the carboxylate group. This motion cannot occur when the dye is bound to the particle surface. Thus, the excited molecules emit from a nuclear configuration that is similar to the ground-state geometry, producing a structured fluorescence spectrum. The dual behavior of the adsorbed dye molecules (electron transfer versus nonradiative decay/fluorescence) is attributed to the existence of two different sites for adsorption at the surface of the TiO2 particles: electron transfer can occur from one site but not the other. (C) 1997 American Institute of Physics. [References: 46]
机译:用约1.00来研究吸附在TiO2半导体颗粒表面的9-蒽羧酸的激发态动力学。 250 fs时间分辨率。瞬态吸收和时间分辨各向异性测量的结合表明,约有76%的光激发染料分子将电子转移到TiO2颗粒上。确定正电子转移反应的时间标度小于或等于1 ps。通过该反应产生的9-蒽-羧酸根自由基阳离子在54 ps的时间尺度上发生反向电子转移。由于不能将电子转移到TiO2的吸附染料分子对瞬态吸收信号的贡献,因此无法更准确地估计正向电子转移反应时间。这些非反应性物质通过非辐射衰变或荧光发射而失活。结合到TiO2颗粒上的染料分子的荧光光谱与溶液中游离染料的荧光光谱非常不同。游离染料具有宽的红移光谱,而吸附的分子具有显示出小的斯托克斯位移的结构化光谱。游离染料荧光光谱中的红移归因于通过羧酸酯基团的扭转运动使激发的电子态稳定。当染料结合到颗粒表面时,不会发生这种运动。因此,被激发的分子从类似于基态几何形状的核构型发射,从而产生结构化的荧光光谱。吸附的染料分子的双重行为(电子转移与非辐射衰变/荧光)归因于在TiO2粒子表面存在两个不同的吸附位点:电子转移可以从一个位点发生,而不能从另一个位点发生。 (C)1997美国物理研究所。 [参考:46]

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