Dec 4, 2024
4:30pm - 4:45pm
Hynes, Level 1, Room 107
Prakriti Kayastha1,Erik Fransson2,Paul Erhart2,Lucy Whalley1
Northumbria University1,Chalmers University of Technology2
Prakriti Kayastha1,Erik Fransson2,Paul Erhart2,Lucy Whalley1
Northumbria University1,Chalmers University of Technology2
Chalcogenide perovskites, particularly BaZrS3, has gained popularity in the last few years due to its great potential as an alternative lead-free photovoltaic absorber material. This is due to promising optoelectronic properties such as defect tolerance, strong dielectric screening, and light absorption [1]. However, some fundamental material physics, in particular polymorphic phase transitions, have not been explored in detail. Experimental studies have given conflicting results with Raman spectroscopy showing no signs of a phase transition[2], whilst XRD studies show an orthorhombic-to-tetragonal phase transition at 800K [3].<br/><br/>In this talk, we will introduce our machine learning potential model trained on perovskite structures with the neuroevolution potential method [4]. Through molecular dynamics calculations, we heat the experimentally reported orthorhombic <i>Pnma</i> phase and observe a first-order phase transition to a tetragonal <i>I4/mcm</i> phase at 610K. Upon further heating, we observe a second-order phase transition from the tetragonal phase to the cubic <i>Pm-3m</i> phase at 880K. We explain the order of these phase transitions through group-subgroup relationships and Landau theory.<br/><br/>Further analysis shows that the phase transitions are mediated through the M and R phonon modes associated with octahedral tilting, as is typically found in perovskite structures [5]. We analyze all possible Glazer tiltings to show that for the BaZrS<sub>3</sub> perovskite only the <i>Pnma --></i><i> I4/mcm --></i><i> Pm-3m</i> phase transition route is accessible through heating. We will also show a temperature-dependent XRD pattern to support further experimental studies.<br/><br/>To end, we will outline how various levels of anharmonicity (harmonic, quasi-harmonic, and fully anharmonic) and exchange-correlation functional (PBEsol and HSE06) impact on our predictions, highlighting some of the subtleties and limitations of each method.<br/><br/><br/>References:<br/><br/>[1] Sopiha et al, Adv. Opt. Mater. 2022 10 2101704.<br/>[2] Ye et al, arXiv: 2402.18957.<br/>[3] Jaykhedkar et al, Inorg. Chem. (2023) 62 12480.<br/>[4] Fan et al, J Chem. Phys. (2022) 157 114801.<br/>[5] Fransson et al, Chem. Mater. (2023) 35 8229.