Impact of the interplay between the organic and inorganic sub-lattices in hybrid halide perovskites
a Trinity College Dublin and CRANN, Dublin
b Qatar Environment and Energy Research Institute,, P.O. Box 5825 Doha
International Conference on Hybrid and Organic Photovoltaics
Proceedings of International Conference on Hybrid and Organic Photovoltaics 2015 (HOPV15)
Proceedings of International Conference on Hybrid and Organic Photovoltaics 2015 (HOPV15)
Roma, Italy, 2015 May 11th - 13th
Organizer: Filippo De Angelis
Poster, Carlo Motta, 051
Publication date: 5th February 2015
Publication date: 5th February 2015
The hybrid halide perovskite CH3NH3PbI3 has enabled solar cells to reach an efficiency close to 20% [1], demonstrating a pace for improvements with no precedents in the solar energy arena [2]. Despite such explosive progress, the microscopic origin behind the success of such material is still debated, with the role played by the organic cations in the light-harvesting process remaining unclear. In this work, density functional theory calculations reveal that the orientation of the organic molecules plays a fundamental role in determining the material electronic properties. Molecular reorientations induce distortions of the inorganic PbI3 cage causing the electronic band edges to shift in reciprocal-space, an effect captured upon inclusion of dispersive forces in the description. As a consequence, inequivalent cation orientations, representing local energy minima, lead to bandstructures displaying either direct and indirect bandgaps [3]. Our observations are compatible with recent photoluminescence measurements. While this subtle effect weakly impacts the mobility of CH3NH3PbI3 [4], it may be a concurrent cause of the slow carrier recombination and of the superior conversion efficiency of CH3NH3PbI3. Our results will be discussed in relation to recent experiments of fast dynamics in this materials class.
Shift of the conduction band minimum from high symmetry point R (left) occurring upon rotation of the methylammonium in the inorganic lattice (right).
[1] Zhou, H. et al. Science 2014, 345, 542–546. [2] Grätzel, M. Nat. Materials 2014, 13, 838–842 [3] Motta, C.; El Mellouhi, F.; Kais, S.; Tabet, N.; Alharbi, F.; Sanvito, S. arXiv:1410.8365 [4] Motta, C.; El Mellouhi, F.; Sanvito, S. arXiv:1411.7904
Shift of the conduction band minimum from high symmetry point R (left) occurring upon rotation of the methylammonium in the inorganic lattice (right).
[1] Zhou, H. et al. Science 2014, 345, 542–546. [2] Grätzel, M. Nat. Materials 2014, 13, 838–842 [3] Motta, C.; El Mellouhi, F.; Kais, S.; Tabet, N.; Alharbi, F.; Sanvito, S. arXiv:1410.8365 [4] Motta, C.; El Mellouhi, F.; Sanvito, S. arXiv:1411.7904
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