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Materials Data on Li2FeBO4 by Materials Project

Li2FeBO4 is beta beryllia-derived structured and crystallizes in the orthorhombic Pmn2_1 space group. The structure is three-dimensional. Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra, corners with four equivalent FeO4 tetrahedra, and corners with four equivalent BO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.93–2.01 Å. Fe3+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with four equivalent BO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.88–1.94 Å. B3+ is bonded to four O2- atoms to form BO4 tetrahedra that share corners with four equivalent FeO4 tetrahedra and corners with eight equivalent LiO4 tetrahedra. There is one shorter (1.49 Å) and three longer (1.51 Å) B–O bond length. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to two equivalent Li1+, one Fe3+, and one B3+ atom to form distorted corner-sharing OLi2FeB tetrahedra. In the second O2- site, O2- is bonded to two equivalent Li1+, one Fe3+, and one B3+ atom to form distorted corner-sharing OLi2FeB trigonal pyramids. In the third O2- site, O2- is bonded to two equivalent Li1+, one Fe3+, and one B3+ atom to form distorted corner-sharing OLi2FeB tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li2FeBO4 by Materials Project

Li2FeBO4 crystallizes in the orthorhombic Pca2_1 space group. The structure is three-dimensional. there are four inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.93–2.47 Å. In the second Li1+ site, Li1+ is bonded to five O2- atoms to form distorted LiO5 trigonal bipyramids that share corners with five BO4 tetrahedra, a cornercorner with one FeO4 trigonal pyramid, and an edgeedge with one FeO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.96–2.15 Å. In the third Li1+ site, Li1+ is bonded in a 3-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 2.03–2.53 Å. In the fourth Li1+ site, Li1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Li–O bond distances ranging from 1.99–2.12 Å. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Fe–O bond distances ranging from 1.90–2.50 Å. In the second Fe3+ site, Fe3+ is bonded to four O2- atoms to form distorted FeO4 trigonal pyramids that share corners with two equivalent BO4 tetrahedra, a cornercorner with one LiO5 trigonal bipyramid, and an edgeedge with one LiO5 trigonal bipyramid. There are a spread of Fe–O bond distances ranging from 1.89–1.96 Å. There are two inequivalent B3+ sites. In the first B3+ site, B3+ is bonded to four O2- atoms to form BO4 tetrahedra that share corners with two equivalent BO4 tetrahedra and corners with two equivalent LiO5 trigonal bipyramids. There are a spread of B–O bond distances ranging from 1.48–1.52 Å. In the second B3+ site, B3+ is bonded to four O2- atoms to form BO4 tetrahedra that share corners with two equivalent BO4 tetrahedra, corners with three equivalent LiO5 trigonal bipyramids, and corners with two equivalent FeO4 trigonal pyramids. There are a spread of B–O bond distances ranging from 1.47–1.51 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe3+, and one B3+ atom. In the second O2- site, O2- is bonded in a 5-coordinate geometry to three Li1+, one Fe3+, and one B3+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to two Li1+ and two B3+ atoms. In the fourth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and two Fe3+ atoms. In the fifth O2- site, O2- is bonded in a distorted trigonal pyramidal geometry to two Li1+ and two B3+ atoms. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+ and three Fe3+ atoms. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe3+, and one B3+ atom. In the eighth O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe3+, and one B3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Li2FeBO4 by Materials Project

Li2FeBO4 crystallizes in the orthorhombic Pna2_1 space group. The structure is three-dimensional. there are two inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Li–O bond distances ranging from 1.93–2.66 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share corners with four equivalent FeO4 tetrahedra and corners with four equivalent BO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.92–2.03 Å. Fe3+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra and corners with four equivalent BO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.88–1.92 Å. B3+ is bonded to four O2- atoms to form BO4 tetrahedra that share corners with four equivalent LiO4 tetrahedra and corners with four equivalent FeO4 tetrahedra. All B–O bond lengths are 1.50 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to three Li1+, one Fe3+, and one B3+ atom. In the second O2- site, O2- is bonded to two Li1+, one Fe3+, and one B3+ atom to form distorted corner-sharing OLi2FeB trigonal pyramids. In the third O2- site, O2- is bonded to two Li1+, one Fe3+, and one B3+ atom to form distorted corner-sharing OLi2FeB tetrahedra. In the fourth O2- site, O2- is bonded to two Li1+, one Fe3+, and one B3+ atom to form distorted corner-sharing OLi2FeB tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Li2FeBO4 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on Li2FeBO4 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on Li2FeBO4 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗