Halide Perovskites: Recent Advances in Optoelectronic Properties from Atomic Scale Modelling
Claudine Katan a, Boubacar Traore a, Mikaël Képénékian a, Laurent Pedesseau b, Jean-Christophe Blancon c, Wanyi Nie c, Hsinhan Tsai c d, Sergei Tretiak c, Constantinos Stoumpos e, Mercouri Kanatzidis e f, Aditya Mohite c g, Jacky Even b
a Institut des Sciences Chimiques de Rennes, CNRS, Université de Rennes 1, Ecole Nationale Supérieure de Chimie de Rennes, INSA Rennes, Rennes, France
b Univ Rennes, INSA Rennes, CNRS, Institut FOTON - UMR6082, France, France
c Los Alamos National Laboratory, US, MS-J567, Los Alamos, NM 87545, United States
d Department of Materials Science and Nanoengineering, Rice University, Houston, US, United States
e Department of Chemistry, Northwestern University, United States, Sheridan Road, 2145, Evanston, United States
f Department of Materials Science and Engineering, Northwestern University, Evanston, Evanston, Illinois, EE. UU., Evanston, United States
g Department of Chemical and Biomolecular Engineering, Rice University, Houston, US, United States
Materials for Sustainable Development Conference (MATSUS)
Proceedings of nanoGe Fall Meeting 2018 (NFM18)
S8 Modelling Perovskite Solar Cells from the Microscale to the Macroscale
Torremolinos, Spain, 2018 October 22nd - 26th
Organizers: Laura Herz, Tze-Chien Sum, Alison Walker and Claudio Quarti
Invited Speaker, Claudine Katan, presentation 166
DOI: https://doi.org/10.29363/nanoge.nfm.2018.166
Publication date: 6th July 2018

Both all inorganic and hybrid halide perovskites have undeniably remarkable characteristics for next-generation photovoltaics, which deserve to be better understood. There are many different perovskite structures that are currently widely explored as absorber materials among which 3D AMX3 and 2D A2 A’n-1 Mn X3n+1 frameworks, where A, A’ are cations, M is a metal, X is a halide. Here, through a couple of recent examples including newly discovered halide perovskite phases [1], we will discuss their optoelectronic properties based on first-principles calculations and semi-empirical modelling. Impact of interfaces [2], structural fluctuations [3], quantum and dielectric confinements [4] on charge carriers and excitons will be inspected. Particular attention will be paid on excitonic effects comparing the results of model calculations with low temperature optical spectroscopy and 60-Tesla magneto-absorption [5]. Theoretical inspection of low energy states associated with electronic states localized on the edges of the perovskite layers [6] will also be shown to provide guidance for the design of new synthetic targets [7] taking advantage of experimentally determined elastic constants [8].

[1] C. M. M. Soe et al. JACS, 139, 16297, 2017; L. Mao et al. JACS, 140, 3775, 2018; X. Li et al. submitted.

[2] W. Nie et al. Adv. Mater. 30, 1703879, 2018.

[3] M. A. Carignano et al. J. Phys. Chem. C, 121, 20729, 2017; A. Marronnier et al. ACS Nano, 12, 3477, 2018; L. Zhou et al. ACS Energy Lett., 3, 787–793, 2018; C. Katan et al. Nature Materials, 17, 377, 2018.

[4] B. Traore et al. ACS Nano, 12, 3321, 2018.

[5] J.-C. Blancon et al. Nature Com. in press (arXiv:1710.07653).

[6] J.-C. Blancon et al. Science, 355, 1288, 2017.

[7] M. Kepenekian et al. arXiv:1801.00704.

[8] A. C. Ferreira et al. arXiv:1801.08701.

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