Disentangling the roles of free-carrier density and mobility in the performance of CH$_{3}$NH$_{3}$PbI$_{3}$ perovskite films

ORAL

Abstract

Apart from broadband absorption of solar radiation, the performance of photovoltaic devices is governed by two parameters carrier mobility and carrier density. They indicate how many and how fast the free carriers drift away from the light­-harvesting medium before loss mechanisms, such as carrier recombination, occur. However, these parameters are usually entangled as a product. Using time­-resolved terahertz spectroscopy, the number density, mobility and quantum yield of charge carriers in a perovskite film have been disentangled. The free­ carrier recombination mechanism and rates were determined, and hence the diffusion length. Our results suggest that perovskite-­based solar cells can perform well even at low temperatures as long as the three-­body recombination has not become predominant.

Authors

  • Elbert Chia

    Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Nanyang Technological University

  • Chan La-o-vorakiat

    Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University

  • M.T. Khuc

    Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University

  • R. Haselsberger

    Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University

  • Maria-Elisabeth Michel-Beyerle

    Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University

  • T. Salim

    School of Materials Science and Engineering, Nanyang Technological University

  • Haibin Su

    School of Materials Science and Engineering, Nanyang Technological University

  • Y.M. Lam

    MSE, NTU, Singapore, School of Materials Science and Engineering, Nanyang Technological University

  • Rudolph A. Marcus

    Noyes Laboratory, California Institute of Technology