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Computational study of Li3BO3 and Li3BN2 I: Electrolyte properties of pure and doped crystals

Both Li3BO3 and Li3BN2 materials have promising properties for use in all-solid-state batteries and other technologies dependent on electrolytes with significant ionic conductivity. As the first of a two-part study, this paper reports the analysis of detailed simulations of Li ion diffusion in the monoclinic forms of these materials. Using both NEB and MD methods, it is clear that Li ion migration via vacancy mechanisms provides the most efficient ion transport in each material. While the results suggest that interstitial defects in these materials do not play a direct role in Li ion migration, their relative stability seems to enhance vacancy production via the formation of Frenkel-type defects. This may partially explain why the Li ion conductivities computed from MD simulations of samples initially containing a single Li ion vacancy are in reasonable agreement with measured values of this work for Li3BO3 and those reported in the literature for poorly crystalline samples of both materials. The possibility of increasing vacancy concentrations by substitutional doping (F for O in Li3BO3 and C for B in Li3BN2) is also examined, finding simulated conductivities comparable to those of the ideal vacancy model.

Li, Yan↗

Materials Data on Li3BN2 by Materials Project

Li3BN2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four N3- atoms. There are a spread of Li–N bond distances ranging from 2.00–2.44 Å. In the second Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four N3- atoms. There are a spread of Li–N bond distances ranging from 2.04–2.51 Å. In the third Li1+ site, Li1+ is bonded to four N3- atoms to form corner-sharing LiN4 tetrahedra. There are a spread of Li–N bond distances ranging from 2.10–2.19 Å. B3+ is bonded in a linear geometry to two N3- atoms. There is one shorter (1.34 Å) and one longer (1.35 Å) B–N bond length. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded in a 1-coordinate geometry to six Li1+ and one B3+ atom. In the second N3- site, N3- is bonded in a 1-coordinate geometry to six Li1+ and one B3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3BN2 by Materials Project

Li3BN2 crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four equivalent N3- atoms to form a mixture of edge and corner-sharing LiN4 tetrahedra. All Li–N bond lengths are 2.13 Å. In the second Li1+ site, Li1+ is bonded in a linear geometry to two equivalent N3- atoms. Both Li–N bond lengths are 1.96 Å. B3+ is bonded in a linear geometry to two equivalent N3- atoms. Both B–N bond lengths are 1.35 Å. N3- is bonded to five Li1+ and one B3+ atom to form a mixture of distorted edge and corner-sharing NLi5B octahedra. The corner-sharing octahedra tilt angles range from 0–68°.

36 MATERIALS SCIENCE↗

Materials Data on Li3BN2 by Materials Project

Li3BN2 crystallizes in the tetragonal I4_1/amd space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a distorted linear geometry to two equivalent N3- atoms. Both Li–N bond lengths are 1.99 Å. In the second Li1+ site, Li1+ is bonded to four equivalent N3- atoms to form a mixture of edge and corner-sharing LiN4 tetrahedra. There are two shorter (2.10 Å) and two longer (2.17 Å) Li–N bond lengths. B3+ is bonded in a linear geometry to two equivalent N3- atoms. Both B–N bond lengths are 1.35 Å. N3- is bonded in a 6-coordinate geometry to five Li1+ and one B3+ atom.

36 MATERIALS SCIENCE↗