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Mg-Ion Conduction in Antiperovskite Solid Electrolytes Revealed by <sup><b>25</b></sup>Mg Ultrahigh Field NMR and First-Principles Calculations

DOE

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Magnesium-ion batteries hold the potential to outperform the energy density of lithium-ion batteries, given the divalent charge carried by each Mg<sup>2+</sup> cation, but remain in an early stage of development. Here, in this study, <sup>25</sup>Mg solid-state nuclear magnetic resonance (ssNMR) is used to gain insight into the local structure and Mg-ion dynamics of candidate Mg-ion solid electrolytes, the antiperovskites Mg<sub>3</sub>SbN and Mg<sub>3</sub>AsN. Using the highest available magnetic field (35.2 T) for high-resolution solid-state NMR, the largest <sup>25</sup>Mg quadrupole coupling constants (C<sub>Q</sub>) yet measured of up to 22 MHz are reported and corroborated by first-principles calculations. Predicted C<sub>Q</sub> values are shown to correlate with the antiperovskite’s tolerance factor; thus, <sup>25</sup>Mg NMR linewidths can report on lattice distortions and phase stability of these antiperovskites. Variable-temperature <sup>25</sup>Mg NMR spectra demonstrate changes at elevated temperatures, ascribed to Mg-ion motional effects. <sup>25</sup>Mg T<sub>1</sub> relaxometry measurements at ultrahigh field reveal a lower activation energy for the more distorted Mg<sub>3</sub>AsN phase, matching computational predictions of a lower energy barrier for Mg<sup>2+</sup> ion migration and suggesting that additional scrutiny of antiperovskites as Mg-ion conductors is warranted. Given the inherent challenges of <sup>25</sup>Mg NMR, this work demonstrates the benefits of combining ultrahigh field NMR spectroscopy, advanced pulse sequences, modern signal processing, and first-principles calculations to facilitate NMR of quadrupolar nuclei as a tool to probe the local structure and ion dynamics in beyond-Li battery materials.. Authors: Halat, David M. [University of California, Berkeley, CA (United States); Colorado School of Mines, Golden, CO (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)] (ORCID:0000000209191689); Liu, Haoyu [Argonne National Laboratory (ANL), Argonne, IL (United States)] (ORCID:0000000267417295); Kim, Kwangnam [University of Michigan, Ann Arbor, MI (United States); Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States). Laboratory for Energy Applications for the Future (LEAF)] (ORCID:0000000311491733); Alexander, Grant C. B. [University of Illinois, Chicago, IL (United States)]; Wang, Xiaoling [Florida State University, Tallahassee, FL (United States). National High Magnetic Field Laboratory (MagLab); California State University, East Bay, Hayward, CA (United States)]. DOE Contract: 89233218CNA000001; AC02-06CH11357; AC52-07NA27344; SC0025712

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