Continuous-time random-walk model of electron transport in nanocrystalline TiO2 electrodes

被引:578
作者
Nelson, J [1 ]
机构
[1] Univ London Imperial Coll Sci Technol & Med, Blackett Lab, London SW7 2BZ, England
来源
PHYSICAL REVIEW B | 1999年 / 59卷 / 23期
关键词
D O I
10.1103/PhysRevB.59.15374
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Electronic junctions made from porous, nanocrystalline TiO2 films in contact with an electrolyte are important for applications such as dye-sensitized solar cells. They exhibit anomalous electron transport properties: extremely slow, nonexponential current and charge recombination transients, and intensity-dependent response times. These features are attributed to a high density of intraband-gap trap states, Most available models of the electron transport are based on the diffusion equation and predict transient and intensity-dt pendant behavior which is not observed. In this paper, a preliminary model of dispersive transport based on the continuous-time random walk is applied to nanocrystalline TiO2 electrodes. Electrons perform a random walk; on a lattice of trap states, each electron moving after a waiting time which is determined by the activation energy of the trap currently occupied. An exponential density of trap states g(E)similar to e(alpha(EC-E)/kT) is used giving rise to a power-law waiting-time distribution, Psi(t)= At-1-alpha. Occupancy of traps is limited to simulate trap filling. The model predicts photocurrents that vary like t(-1-alpha) at long time, and charge recombination transients that are approximately stretched exponential in form. Monte Carlo simulations of photocurrent and charge recombination transients reproduce many of the features that have been observed in practice. Using alpha = 0.37, good quantitative agreement is obtained with measurements of charge recombination kinetics in dye-sensitized TiO2 electrodes under applied bias. The intensity dependence of photocurrent transients can be reproduced. It is also shown that normal diffusive transport, which is represented by Psi(t) = lambda e(-lambda t) fails to explain the observed kinetic behavior. The model is proposed as a starting point for a more refined microscopic treatment in which an experimentally determined density of states can be easily incorporated.
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收藏
页码:15374 / 15380
页数:7
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