Due to high ion conductivity, low cost, and adjustable composition, antiperovskite has attracted attention in solid-state batteries. Ruddlesden-Popper (R-P) antiperovskite is more stable and enhances conductivity. However, systematic theoretical research on R-P antiperovskite is scarce. This study calculates the transport performance, thermodynamic properties, and mechanical properties of R-P antiperovskite LiBr(Li2OHBr)(2) and compares it with H-free LiBr(Li3OBr)(2). Results show that LiBr(Li2OHBr)(2) is prone to defects and increasing LiBr Schottky defects can improve its Li-ion conductivity. The research provides insights into the practical application of R-P antiperovskite in solid-state batteries.
Due to high ion conductivity, low cost, and adjustable composition, antiperovskite has attracted much attention as a potentially useful material in solid-state batteries. Compared with simple antiperovskite, Ruddlesden-Popper (R-P) antiperovskite is an updated material, which is not only more stable but also reported to significantly enhance conductivity when added to simple antiperovskite. However, systematic theoretical research on R-P antiperovskite is scarce, hindering its further development. In this study, the recently reported easily synthesized R-P antiperovskite LiBr(Li2OHBr)(2) is calculated for the first time. Comparative calculations were conducted on the transport performance, thermodynamic properties, and mechanical properties of H-rich LiBr(Li2OHBr)(2) and H-free LiBr(Li3OBr)(2). Our results indicate that due to the presence of protons, LiBr(Li2OHBr)(2) is more prone to defects, and synthesizing more LiBr Schottky defects can improve its Li-ion conductivity. Young's modulus of the LiBr(Li2OHBr)(2) is as low as 30.61 GPa, which is beneficial for its application as a sintering aid. However, the calculated Pugh's ratio (B/G) of 1.28 and 1.50, respectively, indicates that R-P antiperovskites LiBr(Li2OHBr)(2) and LiBr(Li3OBr)(2) exhibit mechanical brittleness, which is not conducive to its application as solid electrolytes. Through quasi-harmonic approximation, we found that the linear thermal expansion coefficient of LiBr(Li2OHBr)(2) is 2.07 x 10(-5) K-1, which is more advantageous in matching electrodes than LiBr(Li3OBr)(2) and even simple antiperovskites. Overall, our research provides comprehensive insights into the practical application of R-P antiperovskite in solid-state batteries.
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