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Electron-Hole Diffusion Lengths Exceeding 1 Micrometer in an Organometal Trihalide Perovskite Absorber

Samuel D. StranksUniversity of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UKGiles E. EperonUniversity of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UKGiulia GranciniCenter for Nano Science and Technology@PoliMi, Istituto Italiano di Tecnologia, Via Giovanni Pascoli 70/3, 20133, Milano, ItalyChristopher MenelaouUniversity of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UKMarcelo J. P. AlcocerCenter for Nano Science and Technology@PoliMi, Istituto Italiano di Tecnologia, Via Giovanni Pascoli 70/3, 20133, Milano, ItalyTomas LeijtensUniversity of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UKLaura M. HerzUniversity of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UKAnnamaria PetrozzaCenter for Nano Science and Technology@PoliMi, Istituto Italiano di Tecnologia, Via Giovanni Pascoli 70/3, 20133, Milano, ItalyHenry J. SnaithUniversity of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, UK
2013en
ABI

Abstract

Organic-inorganic perovskites have shown promise as high-performance absorbers in solar cells, first as a coating on a mesoporous metal oxide scaffold and more recently as a solid layer in planar heterojunction architectures. Here, we report transient absorption and photoluminescence-quenching measurements to determine the electron-hole diffusion lengths, diffusion constants, and lifetimes in mixed halide (CH3NH3PbI(3-x)Cl(x)) and triiodide (CH3NH3PbI3) perovskite absorbers. We found that the diffusion lengths are greater than 1 micrometer in the mixed halide perovskite, which is an order of magnitude greater than the absorption depth. In contrast, the triiodide absorber has electron-hole diffusion lengths of ~100 nanometers. These results justify the high efficiency of planar heterojunction perovskite solar cells and identify a critical parameter to optimize for future perovskite absorber development.

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