Abstract

The temperature and photoexcitation density dependences of the electron transport dynamics in electrolyte-filled mesoporous ${\mathrm{TiO}}_{2}$ nanoparticle films were investigated by transient photocurrent measurements. The thermal activation energy of the diffusion coefficient of photogenerated electrons ranged from 0.19--0.27 eV, depending on the specific sample studied. The diffusion coefficient also depends strongly on the photoexcitation density; however, the activation energy has little, if any, dependence on the photoexcitation density. The light intensity dependence can be used to infer temperature-independent dispersion parameters in the range 0.3--0.5. These results are inconsistent with the widely used transport model that assumes multiple trapping of electrons in an exponential conduction-band tail. We can also exclude a model allowing for widening of a band tail with increased temperature. Our results suggest that structural, not energetic, disorder limits electron transport in mesoporous ${\mathrm{TiO}}_{2}$. The analogy between this material and others in which charge transport is limited by structural disorder is discussed.

Highlights

  • IntroductionA second remarkable example of a porous semiconductor is porous titania, which is the basis of an efficient, dyesensitized solar cell

  • The temperature and photoexcitation density dependences of the electron transport dynamics in electrolytefilled mesoporous TiO2 nanoparticle films were investigated by transient photocurrent measurements

  • The thermal activation energy of the diffusion coefficient of photogenerated electrons ranged from 0.19–0.27 eV, depending on the specific sample studied

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Summary

Introduction

A second remarkable example of a porous semiconductor is porous titania, which is the basis of an efficient, dyesensitized solar cell.. A second remarkable example of a porous semiconductor is porous titania, which is the basis of an efficient, dyesensitized solar cell.3,4 In this material, a mesoporous TiO2 film is prepared by sintering of titania particles with a typical diameter around 20 nm. The resulting, bicontinuous porous material separates the transport pathways of electrons from their counterchargesions or holes. This separation is valuable for solar cell applications since it inhibits the recombination of photogenerated electrons with the countercharges

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