Abstract

Organometal halide perovskites are attracting great attention as promising material for solar cells because of their high power conversion efficiency. The high performance has been attributed to the existence of free charge carriers and their large diffusion lengths, but the nature of carrier transport at the atomistic level remains elusive. Here, nonadiabatic quantum molecular dynamics simulations elucidate the mechanisms underlying the excellent free-carrier transport in CH3NH3PbI3. Pb and I sublattices act as disjunct pathways for rapid and balanced transport of photoexcited electrons and holes, respectively, while minimizing efficiency-degrading charge recombination. On the other hand, CH3NH3 sublattice quickly screens out electrostatic electron-hole attraction to generate free carriers within 1 ps. Together this nano-architecture lets photoexcited electrons and holes dissociate instantaneously and travel far away to be harvested before dissipated as heat. This work provides much needed structure-property relationships and time-resolved information that potentially lead to rational design of efficient solar cells.

Highlights

  • Organometal halide perovskites are attracting great attention as promising material for solar cells because of their high power conversion efficiency

  • Organometal halide perovskites such as methylammonium lead iodide (CH3NH3PbI3 or MAPbI3)[1] are attracting a great deal of attention as promising material for solar cells because of their high power conversion efficiency[2,3,4,5,6] exceeding 20%7,8

  • The high performance has generally been attributed to excellent transport properties of photoexcited charge carriers[7,8]

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Summary

Introduction

Organometal halide perovskites are attracting great attention as promising material for solar cells because of their high power conversion efficiency. To study photoexcited charge-carrier dynamics, we performed NAQMD simulations.

Results
Conclusion
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