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Materials Data on LiFe2(CO3)4 by Materials Project

LiFe2(CO3)4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. Li is bonded in a 3-coordinate geometry to five O atoms. There are a spread of Li–O bond distances ranging from 1.96–2.62 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded in a distorted pentagonal pyramidal geometry to six O atoms. There are a spread of Fe–O bond distances ranging from 2.00–2.16 Å. In the second Fe site, Fe is bonded in a pentagonal pyramidal geometry to six O atoms. There are a spread of Fe–O bond distances ranging from 2.00–2.07 Å. There are four inequivalent C sites. In the first C site, C is bonded in a trigonal planar geometry to three O atoms. There is one shorter (1.29 Å) and two longer (1.30 Å) C–O bond length. In the second C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.31 Å. In the third C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.31 Å. In the fourth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.28–1.31 Å. There are twelve inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to one Li, one Fe, and one C atom. In the second O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the third O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the fourth O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the fifth O site, O is bonded in a bent 120 degrees geometry to one Fe and one C atom. In the sixth O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the seventh O site, O is bonded in a bent 120 degrees geometry to one Fe and one C atom. In the eighth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the ninth O site, O is bonded in a 2-coordinate geometry to one Li, one Fe, and one C atom. In the tenth O site, O is bonded in a 1-coordinate geometry to one Fe and one C atom. In the eleventh O site, O is bonded in a distorted T-shaped geometry to one Li, one Fe, and one C atom. In the twelfth O site, O is bonded in a 2-coordinate geometry to one Li, one Fe, and one C atom.

36 MATERIALS SCIENCE↗

Materials Data on LiFe2(CO3)4 by Materials Project

LiFe2(CO3)4 crystallizes in the triclinic P1 space group. The structure is three-dimensional. Li is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Li–O bond distances ranging from 1.96–2.51 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded in an octahedral geometry to six O atoms. There are a spread of Fe–O bond distances ranging from 2.03–2.10 Å. In the second Fe site, Fe is bonded in an octahedral geometry to six O atoms. There are a spread of Fe–O bond distances ranging from 1.98–2.10 Å. There are four inequivalent C sites. In the first C site, C is bonded in a trigonal planar geometry to three O atoms. There is one shorter (1.29 Å) and two longer (1.30 Å) C–O bond length. In the second C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.31 Å. In the third C site, C is bonded in a trigonal planar geometry to three O atoms. There is one shorter (1.27 Å) and two longer (1.31 Å) C–O bond length. In the fourth C site, C is bonded in a trigonal planar geometry to three O atoms. There is two shorter (1.29 Å) and one longer (1.31 Å) C–O bond length. There are twelve inequivalent O sites. In the first O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the second O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the third O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the fourth O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the fifth O site, O is bonded in a bent 120 degrees geometry to one Fe and one C atom. In the sixth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the seventh O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the eighth O site, O is bonded in a bent 120 degrees geometry to one Fe and one C atom. In the ninth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the tenth O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the eleventh O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the twelfth O site, O is bonded in an L-shaped geometry to one Fe and one C atom.

36 MATERIALS SCIENCE↗

Materials Data on Li3Fe2(CO4)2 by Materials Project

Li3Fe2(CO4)2 crystallizes in the monoclinic Pc space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share a cornercorner with one LiO4 tetrahedra, a cornercorner with one FeO4 tetrahedra, corners with two equivalent LiO4 trigonal pyramids, and an edgeedge with one FeO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.91–2.09 Å. In the second Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 tetrahedra that share a cornercorner with one LiO4 tetrahedra, corners with four FeO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Li–O bond distances ranging from 1.94–2.11 Å. In the third Li1+ site, Li1+ is bonded to four O2- atoms to form LiO4 trigonal pyramids that share a cornercorner with one FeO4 tetrahedra, corners with three LiO4 tetrahedra, an edgeedge with one LiO4 tetrahedra, and an edgeedge with one FeO4 tetrahedra. There are a spread of Li–O bond distances ranging from 1.93–2.18 Å. There are two inequivalent Fe+2.50+ sites. In the first Fe+2.50+ site, Fe+2.50+ is bonded to four O2- atoms to form FeO4 tetrahedra that share corners with two equivalent LiO4 tetrahedra, corners with two equivalent FeO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, and an edgeedge with one LiO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.82–2.02 Å. In the second Fe+2.50+ site, Fe+2.50+ is bonded to four O2- atoms to form distorted FeO4 tetrahedra that share corners with two equivalent FeO4 tetrahedra, corners with three LiO4 tetrahedra, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Fe–O bond distances ranging from 1.92–2.26 Å. There are two inequivalent C4+ sites. In the first C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There are a spread of C–O bond distances ranging from 1.28–1.32 Å. In the second C4+ site, C4+ is bonded in a trigonal planar geometry to three O2- atoms. There is one shorter (1.26 Å) and two longer (1.32 Å) C–O bond length. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded to three Li1+ and one C4+ atom to form edge-sharing OLi3C tetrahedra. In the second O2- site, O2- is bonded in a 3-coordinate geometry to one Li1+, one Fe+2.50+, and one C4+ atom. In the third O2- site, O2- is bonded in a bent 120 degrees geometry to one Fe+2.50+ and one C4+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Li1+ and two Fe+2.50+ atoms. In the fifth O2- site, O2- is bonded to two Li1+ and two Fe+2.50+ atoms to form distorted edge-sharing OLi2Fe2 trigonal pyramids. In the sixth O2- site, O2- is bonded in a trigonal planar geometry to one Li1+, one Fe+2.50+, and one C4+ atom. In the seventh O2- site, O2- is bonded in a 4-coordinate geometry to two Li1+, one Fe+2.50+, and one C4+ atom. In the eighth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Li1+ and one C4+ atom.

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Materials Data on Li2FeCO4 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

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Materials Data on Li17Fe4(CO3)16 by Materials Project

Li17Fe4(CO3)16 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are seventeen inequivalent Li sites. In the first Li site, Li is bonded to five O atoms to form distorted LiO5 trigonal bipyramids that share a cornercorner with one FeO6 octahedra, a cornercorner with one LiO5 square pyramid, an edgeedge with one LiO4 tetrahedra, and an edgeedge with one LiO5 trigonal bipyramid. The corner-sharing octahedral tilt angles are 62°. There are a spread of Li–O bond distances ranging from 2.06–2.29 Å. In the second Li site, Li is bonded to five O atoms to form LiO5 square pyramids that share corners with two FeO6 octahedra, a cornercorner with one LiO5 trigonal bipyramid, and an edgeedge with one LiO4 trigonal pyramid. The corner-sharing octahedra tilt angles range from 73–79°. There are a spread of Li–O bond distances ranging from 2.00–2.19 Å. In the third Li site, Li is bonded to five O atoms to form LiO5 square pyramids that share corners with two FeO6 octahedra and a cornercorner with one LiO4 tetrahedra. The corner-sharing octahedra tilt angles range from 74–81°. There are a spread of Li–O bond distances ranging from 2.02–2.18 Å. In the fourth Li site, Li is bonded to four O atoms to form distorted LiO4 trigonal pyramids that share corners with two LiO4 tetrahedra and an edgeedge with one LiO5 square pyramid. There are a spread of Li–O bond distances ranging from 1.93–2.07 Å. In the fifth Li site, Li is bonded in a distorted rectangular see-saw-like geometry to four O atoms. There are a spread of Li–O bond distances ranging from 2.01–2.09 Å. In the sixth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share a cornercorner with one LiO4 trigonal pyramid, an edgeedge with one FeO6 octahedra, and an edgeedge with one LiO5 trigonal bipyramid. There are a spread of Li–O bond distances ranging from 1.96–2.07 Å. In the seventh Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share a cornercorner with one LiO4 trigonal pyramid and an edgeedge with one FeO6 octahedra. There are a spread of Li–O bond distances ranging from 1.96–2.05 Å. In the eighth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share corners with three FeO6 octahedra and a cornercorner with one LiO5 square pyramid. The corner-sharing octahedra tilt angles range from 17–66°. There are a spread of Li–O bond distances ranging from 1.99–2.16 Å. In the ninth Li site, Li is bonded in a 4-coordinate geometry to five O atoms. There are a spread of Li–O bond distances ranging from 1.98–2.55 Å. In the tenth Li site, Li is bonded to four O atoms to form distorted LiO4 tetrahedra that share a cornercorner with one LiO5 trigonal bipyramid and an edgeedge with one FeO6 octahedra. There are a spread of Li–O bond distances ranging from 1.96–2.05 Å. In the eleventh Li site, Li is bonded to four O atoms to form LiO4 trigonal pyramids that share a cornercorner with one LiO5 trigonal bipyramid, an edgeedge with one FeO6 octahedra, and an edgeedge with one LiO5 trigonal bipyramid. There are a spread of Li–O bond distances ranging from 1.97–2.08 Å. In the twelfth Li site, Li is bonded in a distorted see-saw-like geometry to four O atoms. There are a spread of Li–O bond distances ranging from 1.94–2.13 Å. In the thirteenth Li site, Li is bonded to five O atoms to form distorted LiO5 trigonal bipyramids that share a cornercorner with one LiO4 tetrahedra, a cornercorner with one LiO4 trigonal pyramid, and an edgeedge with one LiO5 square pyramid. There are a spread of Li–O bond distances ranging from 1.98–2.30 Å. In the fourteenth Li site, Li is bonded to five O atoms to form LiO5 square pyramids that share corners with two FeO6 octahedra. The corner-sharing octahedra tilt angles range from 75–80°. There are a spread of Li–O bond distances ranging from 2.01–2.19 Å. In the fifteenth Li site, Li is bonded to five O atoms to form LiO5 square pyramids that share corners with two FeO6 octahedra, a cornercorner with one LiO5 trigonal bipyramid, and an edgeedge with one LiO5 trigonal bipyramid. The corner-sharing octahedra tilt angles range from 73–76°. There are a spread of Li–O bond distances ranging from 2.03–2.26 Å. In the sixteenth Li site, Li is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Li–O bond distances ranging from 2.05–2.43 Å. In the seventeenth Li site, Li is bonded to five O atoms to form LiO5 trigonal bipyramids that share a cornercorner with one FeO6 octahedra, a cornercorner with one LiO5 square pyramid, an edgeedge with one LiO5 trigonal bipyramid, and an edgeedge with one LiO4 trigonal pyramid. The corner-sharing octahedral tilt angles are 63°. There are a spread of Li–O bond distances ranging from 2.06–2.28 Å. There are four inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form distorted FeO6 octahedra that share corners with two LiO5 square pyramids, a cornercorner with one LiO4 tetrahedra, a cornercorner with one LiO5 trigonal bipyramid, and an edgeedge with one LiO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 2.05–2.10 Å. In the second Fe site, Fe is bonded to six O atoms to form distorted FeO6 octahedra that share corners with two LiO5 square pyramids, a cornercorner with one LiO4 tetrahedra, and an edgeedge with one LiO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 2.00–2.16 Å. In the third Fe site, Fe is bonded to six O atoms to form distorted FeO6 octahedra that share corners with two LiO5 square pyramids and an edgeedge with one LiO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 2.05–2.09 Å. In the fourth Fe site, Fe is bonded to six O atoms to form distorted FeO6 octahedra that share corners with two LiO5 square pyramids, a cornercorner with one LiO4 tetrahedra, a cornercorner with one LiO5 trigonal bipyramid, and an edgeedge with one LiO4 trigonal pyramid. There are a spread of Fe–O bond distances ranging from 2.02–2.15 Å. There are sixteen inequivalent C sites. In the first C site, C is bonded in a trigonal planar geometry to three O atoms. There is two shorter (1.28 Å) and one longer (1.32 Å) C–O bond length. In the second C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.32 Å. In the third C site, C is bonded in a trigonal planar geometry to three O atoms. There is two shorter (1.27 Å) and one longer (1.34 Å) C–O bond length. In the fourth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.28–1.31 Å. In the fifth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.26–1.32 Å. In the sixth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.28–1.31 Å. In the seventh C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.32 Å. In the eighth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.26–1.32 Å. In the ninth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.32 Å. In the tenth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.26–1.32 Å. In the eleventh C site, C is bonded in a trigonal planar geometry to three O atoms. There is one shorter (1.26 Å) and two longer (1.31 Å) C–O bond length. In the twelfth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.28–1.31 Å. In the thirteenth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.33 Å. In the fourteenth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.34 Å. In the fifteenth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.26–1.32 Å. In the sixteenth C site, C is bonded in a trigonal planar geometry to three O atoms. There are a spread of C–O bond distances ranging from 1.27–1.32 Å. There are forty-eight inequivalent O sites. In the first O site, O is bonded in a 3-coordinate geometry to two Li and one C atom. In the second O site, O is bonded in a distorted bent 120 degrees geometry to one Li and one C atom. In the third O site, O is bonded in a bent 120 degrees geometry to one Li and one C atom. In the fourth O site, O is bonded in a 1-coordinate geometry to two Li and one C atom. In the fifth O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the sixth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the seventh O site, O is bonded in a trigonal planar geometry to two Li and one C atom. In the eighth O site, O is bonded to three Li and one C atom to form distorted edge-sharing OLi3C tetrahedra. In the ninth O site, O is bonded in a distorted T-shaped geometry to two Li and one C atom. In the tenth O site, O is bonded in a distorted T-shaped geometry to two Li and one C atom. In the eleventh O site, O is bonded to two Li, one Fe, and one C atom to form distorted edge-sharing OLi2FeC tetrahedra. In the twelfth O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the thirteenth O site, O is bonded in a distorted trigonal planar geometry to two Li and one C atom. In the fourteenth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the fifteenth O site, O is bonded in a distorted rectangular see-saw-like geometry to three Li and one C atom. In the sixteenth O site, O is bonded in a distorted trigonal non-coplanar geometry to one Li, one Fe, and one C atom. In the seventeenth O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the eighteenth O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the nineteenth O site, O is bonded in a distorted trigonal planar geometry to two Li and one C atom. In the twentieth O site, O is bonded in a 3-coordinate geometry to two Li and one C atom. In the twenty-first O site, O is bonded in a distorted trigonal non-coplanar geometry to one Li, one Fe, and one C atom. In the twenty-second O site, O is bonded in a distorted T-shaped geometry to one Li, one Fe, and one C atom. In the twenty-third O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the twenty-fourth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the twenty-fifth O site, O is bonded in an L-shaped geometry to one Fe and one C atom. In the twenty-sixth O site, O is bonded in a 3-coordinate geometry to one Li, one Fe, and one C atom. In the twenty-seventh O site, O is bonded in a distorted trigonal non-coplanar geometry to one Li, one Fe, and one C atom. In the twenty-eighth O site, O is bonded in a distorted T-shaped geometry to one Li, one Fe, and one C atom. In the twenty-ninth O site, O is bonded in a distorted T-shaped geometry to two Li and one C atom. In the thirtieth O site, O is bonded in a distorted trigonal planar geometry to two Li and one C atom. In the thirty-first O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the thirty-second O site, O is bonded in a distorted trigonal planar geometry to one Li, one Fe, and one C atom. In the thirty-third O site, O is bonded in a 3-coordinate geometry to two Li, one Fe, and one C atom. In the thirty-fo

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Materials Data on Li2Fe(CO3)2 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 LiFe2(CO3)4 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 LiFe(CO3)2 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↗