Abstract
Most metal halide perovskites (MHPs) which under ambient conditions crystallize in a tetragonal or cubic phase exhibit a fairly linear increase of the fundamental gap with increasing temperature, in frank contrast to other conventional semiconductors. Though valid in general for MHPs, it has been shown for the archetypal perovskite MAPbI3 (MA stands for methylammonium) that such a behavior is due to an almost equal footing of the effects of thermal expansion on the electronic states and the temperature-induced gap renormalization due to the electron–phonon interaction. Here, the influence of the incorporation of small amounts of Cs on the gap renormalization was investigated in two CsxMA1–xPbI3 single crystals (x = 0.05 and 0.1). Strikingly, from ambient to a temperature Ton of 250–280 K, the slope of the linear temperature dependence of the energy gap for both Cs-containing samples is almost half that for pure MAPbI3. Below Ton and within the stability range of the tetragonal phase, the slope recovers the value of MAPbI3. Based on density functional theory calculations, this surprising behavior is explained as being due to the appearance of an additional electron–phonon coupling mechanism ascribed to dynamic tilting of the PbI6 octahedrons. The latter is activated by the translational dynamics of the Cs cations between equivalent potential minima inside the inorganic cage voids, which is unfolded above the onset temperature Ton. These results provide further evidence of the key role that the A-site cation dynamics plays in the optoelectronic properties of this fascinating class of materials.
Original language | English |
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Pages (from-to) | 22817-22826 |
Number of pages | 10 |
Journal | Journal of Physical Chemistry C |
Volume | 127 |
Issue number | 46 |
Early online date | 9 Nov 2023 |
DOIs | |
Publication status | Published - 23 Nov 2023 |
Bibliographical note
Funding Information:The Spanish ”Ministerio de Ciencia e Innovación (MICINN)” is gratefully acknowledged for its support through grant CEX2019-000917 S (FUNFUTURE) in the framework of the Spanish Severo Ochoa Centre of Excellence program and the AEI/FEDER(UE) grants PGC2018-095411-B-100 (RAINBOW) and PID2021-128924OB-I00 (ISOSCELLES). The authors also thank the Catalan agency AGAUR for grant 2021-SGR-00444 and the National Network ”Red Perovskitas” (MICINN funded). K.X. acknowledges a fellowship (CSC201806950006) from China Scholarship Council and the PhD programme in Materials Science from Universitat Autònoma de Barcelona in which he was enrolled. B.C. thanks the EPSRC for PhD studentship funding via the University of Bath, CSCT CDT (EP/G03768 X/1). We would also like to thank ISIS for the award of beamtime under Proposal RB1610285(ISIS).
Publisher Copyright:
© 2023 American Chemical Society.