Local Field Effects on Electron Transport in Nanostructured TiO<sub>2</sub> Revealed by Terahertz Spectroscopy

E. Hendry, Mattijs Koeberg, Brian C. O’Regan, Mischa Bonn

Nano Letters · 2006 · 370 citations · 17 references

Concepts

TL;DR

The study investigates electron mobilities in nanoporous and single‑crystal TiO₂ using terahertz time‑domain spectroscopy. Ultrafast terahertz spectroscopy determines electron mobility after carrier thermalization with the lattice but before equilibration with defect trapping states. Measured mobilities of 1 cm²/(V s) for single‑crystal rutile and 10⁻² cm²/(V s) for porous TiO₂ reveal a morphology‑dependent transport limited by local field effects, as explained by Maxwell‑Garnett theory, and indicate that mobility is not a direct proxy for the diffusion coefficient.

Abstract

We study electron mobilities in nanoporous and single-crystal titanium dioxide with terahertz time domain spectroscopy. This ultrafast technique allows the determination of the electron mobility after carrier thermalization with the lattice but before equilibration with defect trapping states. The mobilities reported here for single-crystal rutile (1 cm2/(V s)) and porous TiO2 (10(-2) cm2/(V s)) therefore represent upper limits for electron transport at room temperature for defect-free materials. The large difference in mobility between bulk and porous samples is explained using Maxwell-Garnett effective medium theory. These results demonstrate that electron mobility is strongly dependent on the material morphology in nanostructured polar materials due to local field effects and cannot be used as a direct measure of the diffusion coefficient.

References

17