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DOE OSTI2020

Materials Data on La3Cd(FeO3)4 by Materials Project

La3Cd(FeO3)4 is Orthorhombic Perovskite-derived structured and crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are three inequivalent La sites. In the first La site, La is bonded in a 3-coordinate geometry to eight O atoms. There are a spread of La–O bond distances ranging from 2.41–2.83 Å. In the second La site, La is bonded in a 12-coordinate geometry to eight O atoms. There are a spread of La–O bond distances ranging from 2.39–2.86 Å. In the third La site, La is bonded in a 9-coordinate geometry to eight O atoms. There are a spread of La–O bond distances ranging from 2.41–2.74 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form corner-sharing FeO6 octahedra. The corner-sharing octahedra tilt angles range from 22–29°. There are a spread of Fe–O bond distances ranging from 1.99–2.07 Å. In the second Fe site, Fe is bonded to six O atoms to form corner-sharing FeO6 octahedra. The corner-sharing octahedra tilt angles range from 22–31°. There are a spread of Fe–O bond distances ranging from 2.00–2.07 Å. Cd is bonded in a 4-coordinate geometry to four O atoms. There are a spread of Cd–O bond distances ranging from 2.29–2.45 Å. There are eight inequivalent O sites. In the first O site, O is bonded in a 4-coordinate geometry to one La, two equivalent Fe, and one Cd atom. In the second O site, O is bonded in a 4-coordinate geometry to one La, two equivalent Fe, and one Cd atom. In the third O site, O is bonded in a 4-coordinate geometry to two La and two equivalent Fe atoms. In the fourth O site, O is bonded in a 4-coordinate geometry to two La and two equivalent Fe atoms. In the fifth O site, O is bonded in a 3-coordinate geometry to two La and two Fe atoms. In the sixth O site, O is bonded in a 5-coordinate geometry to two La, two Fe, and one Cd atom. In the seventh O site, O is bonded in a 5-coordinate geometry to three La and two Fe atoms. In the eighth O site, O is bonded to two La and two Fe atoms to form distorted edge-sharing OLa2Fe2 trigonal pyramids.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Sr4Ca(FeO3)5 by Materials Project

Sr4Ca(FeO3)5 is (Cubic) Perovskite-derived structured and crystallizes in the tetragonal P4/m space group. The structure is three-dimensional. Sr is bonded to twelve O atoms to form SrO12 cuboctahedra that share corners with three equivalent CaO12 cuboctahedra, corners with nine equivalent SrO12 cuboctahedra, a faceface with one CaO12 cuboctahedra, faces with five equivalent SrO12 cuboctahedra, and faces with eight FeO6 octahedra. There are nine shorter (2.76 Å) and three longer (2.78 Å) Sr–O bond lengths. Ca is bonded to twelve O atoms to form CaO12 cuboctahedra that share corners with twelve equivalent SrO12 cuboctahedra, faces with two equivalent CaO12 cuboctahedra, faces with four equivalent SrO12 cuboctahedra, and faces with eight equivalent FeO6 octahedra. All Ca–O bond lengths are 2.75 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six FeO6 octahedra and faces with eight equivalent SrO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. There is two shorter (1.95 Å) and four longer (1.96 Å) Fe–O bond length. In the second Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six FeO6 octahedra, faces with two equivalent CaO12 cuboctahedra, and faces with six equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–1°. There is four shorter (1.95 Å) and two longer (1.96 Å) Fe–O bond length. There are five inequivalent O sites. In the first O site, O is bonded to four equivalent Sr and two equivalent Fe atoms to form distorted OSr4Fe2 octahedra that share corners with twenty-two OSr4Fe2 octahedra, edges with four equivalent OSr3CaFe2 octahedra, and faces with eight equivalent OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the second O site, O is bonded to three equivalent Sr, one Ca, and two equivalent Fe atoms to form distorted OSr3CaFe2 octahedra that share corners with twenty-two OSr4Fe2 octahedra, edges with four OSr4Fe2 octahedra, and faces with eight OSr2Ca2Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the third O site, O is bonded to four equivalent Sr and two Fe atoms to form distorted OSr4Fe2 octahedra that share corners with twenty-two OSr2Ca2Fe2 octahedra, edges with four OSr2Ca2Fe2 octahedra, and faces with eight OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the fourth O site, O is bonded to two equivalent Sr, two equivalent Ca, and two equivalent Fe atoms to form distorted OSr2Ca2Fe2 octahedra that share corners with twenty-two OSr4Fe2 octahedra, edges with four OSr2Ca2Fe2 octahedra, and faces with eight OSr2Ca2Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the fifth O site, O is bonded to four equivalent Sr and two equivalent Fe atoms to form distorted OSr4Fe2 octahedra that share corners with twenty-two OSr2Ca2Fe2 octahedra, edges with four OSr4Fe2 octahedra, and faces with eight OSr2Ca2Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on BaSr4(FeO3)5 by Materials Project

BaSr4(FeO3)5 is (Cubic) Perovskite-derived structured and crystallizes in the orthorhombic Cmmm space group. The structure is three-dimensional. Ba is bonded to twelve O atoms to form BaO12 cuboctahedra that share corners with two equivalent BaO12 cuboctahedra, corners with ten SrO12 cuboctahedra, faces with two equivalent BaO12 cuboctahedra, faces with four equivalent SrO12 cuboctahedra, and faces with eight FeO6 octahedra. There are a spread of Ba–O bond distances ranging from 2.79–2.84 Å. There are three inequivalent Sr sites. In the first Sr site, Sr is bonded to twelve O atoms to form SrO12 cuboctahedra that share corners with four equivalent BaO12 cuboctahedra, corners with eight SrO12 cuboctahedra, faces with two equivalent BaO12 cuboctahedra, faces with four SrO12 cuboctahedra, and faces with eight FeO6 octahedra. There are a spread of Sr–O bond distances ranging from 2.76–2.80 Å. In the second Sr site, Sr is bonded to twelve O atoms to form SrO12 cuboctahedra that share a cornercorner with one BaO12 cuboctahedra, corners with eleven SrO12 cuboctahedra, faces with six SrO12 cuboctahedra, and faces with eight FeO6 octahedra. There are a spread of Sr–O bond distances ranging from 2.74–2.79 Å. In the third Sr site, Sr is bonded to twelve O atoms to form SrO12 cuboctahedra that share a cornercorner with one BaO12 cuboctahedra, corners with eleven SrO12 cuboctahedra, faces with six SrO12 cuboctahedra, and faces with eight FeO6 octahedra. There are a spread of Sr–O bond distances ranging from 2.74–2.79 Å. There are three inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six FeO6 octahedra, faces with two equivalent BaO12 cuboctahedra, and faces with six SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–3°. There is four shorter (1.97 Å) and two longer (1.98 Å) Fe–O bond length. In the second Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six FeO6 octahedra and faces with eight SrO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. There is two shorter (1.96 Å) and four longer (1.97 Å) Fe–O bond length. In the third Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six FeO6 octahedra, faces with four equivalent BaO12 cuboctahedra, and faces with four equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 0–3°. There is two shorter (1.97 Å) and four longer (1.99 Å) Fe–O bond length. There are seven inequivalent O sites. In the first O site, O is bonded to two equivalent Ba, two equivalent Sr, and two equivalent Fe atoms to form distorted OBa2Sr2Fe2 octahedra that share corners with twenty-two OBa2Sr2Fe2 octahedra, edges with four OBaSr3Fe2 octahedra, and faces with eight equivalent OBa2Sr2Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the second O site, O is bonded to one Ba, three Sr, and two equivalent Fe atoms to form distorted OBaSr3Fe2 octahedra that share corners with twenty-two OBaSr3Fe2 octahedra, edges with four OBa2Sr2Fe2 octahedra, and faces with eight OBa2Sr2Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. There are one shorter (2.74 Å) and two longer (2.79 Å) O–Sr bond lengths. Both O–Fe bond lengths are 1.97 Å. In the third O site, O is bonded to two equivalent Ba, two equivalent Sr, and two Fe atoms to form a mixture of distorted face, edge, and corner-sharing OBa2Sr2Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–61°. In the fourth O site, O is bonded to four Sr and two equivalent Fe atoms to form a mixture of distorted face, edge, and corner-sharing OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the fifth O site, O is bonded to four Sr and two Fe atoms to form a mixture of distorted face, edge, and corner-sharing OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the sixth O site, O is bonded to one Ba, three Sr, and two equivalent Fe atoms to form a mixture of distorted face, edge, and corner-sharing OBaSr3Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°. In the seventh O site, O is bonded to four Sr and two equivalent Fe atoms to form distorted OSr4Fe2 octahedra that share corners with twenty-two OBa2Sr2Fe2 octahedra, edges with four OBaSr3Fe2 octahedra, and faces with eight OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–60°.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on La3Al(FeO3)4 by Materials Project

La3Al(FeO3)4 crystallizes in the monoclinic Pm space group. The structure is three-dimensional. there are three inequivalent La3+ sites. In the first La3+ site, La3+ is bonded in a 8-coordinate geometry to eight O2- atoms. There are a spread of La–O bond distances ranging from 2.38–2.70 Å. In the second La3+ site, La3+ is bonded in a 4-coordinate geometry to eight O2- atoms. There are a spread of La–O bond distances ranging from 2.32–2.88 Å. In the third La3+ site, La3+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of La–O bond distances ranging from 2.43–2.91 Å. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to six O2- atoms to form distorted FeO6 octahedra that share corners with six FeO6 octahedra and corners with two equivalent AlO4 tetrahedra. The corner-sharing octahedra tilt angles range from 26–48°. There are a spread of Fe–O bond distances ranging from 1.95–2.47 Å. In the second Fe3+ site, Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six FeO6 octahedra and corners with two equivalent AlO4 tetrahedra. The corner-sharing octahedra tilt angles range from 25–48°. There are a spread of Fe–O bond distances ranging from 1.99–2.12 Å. Al3+ is bonded to four O2- atoms to form distorted AlO4 tetrahedra that share corners with eight FeO6 octahedra. The corner-sharing octahedra tilt angles range from 63–73°. There are a spread of Al–O bond distances ranging from 1.85–1.91 Å. There are eight inequivalent O2- sites. In the first O2- site, O2- is bonded to two La3+ and two Fe3+ atoms to form a mixture of distorted corner and edge-sharing OLa2Fe2 tetrahedra. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two La3+, two Fe3+, and one Al3+ atom. In the third O2- site, O2- is bonded in a 5-coordinate geometry to three La3+ and two Fe3+ atoms. In the fourth O2- site, O2- is bonded to two La3+ and two Fe3+ atoms to form a mixture of distorted corner and edge-sharing OLa2Fe2 trigonal pyramids. In the fifth O2- site, O2- is bonded in a 4-coordinate geometry to one La3+, two equivalent Fe3+, and one Al3+ atom. In the sixth O2- site, O2- is bonded in a 4-coordinate geometry to one La3+, two equivalent Fe3+, and one Al3+ atom. In the seventh O2- site, O2- is bonded to two La3+ and two equivalent Fe3+ atoms to form a mixture of distorted corner and edge-sharing OLa2Fe2 tetrahedra. In the eighth O2- site, O2- is bonded in a 3-coordinate geometry to three La3+ and two equivalent Fe3+ atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Sr2Nd(FeO3)3 by Materials Project

Sr2Nd(FeO3)3 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. Sr is bonded to twelve O atoms to form distorted SrO12 cuboctahedra that share corners with nine equivalent SrO12 cuboctahedra, faces with three equivalent SrO12 cuboctahedra, and faces with eight FeO6 octahedra. There are a spread of Sr–O bond distances ranging from 2.56–3.02 Å. Nd is bonded in a 12-coordinate geometry to twelve O atoms. There are a spread of Nd–O bond distances ranging from 2.47–3.11 Å. There are two inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six FeO6 octahedra and faces with five equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 8–19°. There are a spread of Fe–O bond distances ranging from 1.95–1.99 Å. In the second Fe site, Fe is bonded to six O atoms to form FeO6 octahedra that share corners with six equivalent FeO6 octahedra and faces with six equivalent SrO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 8–15°. There are a spread of Fe–O bond distances ranging from 1.95–1.98 Å. There are five inequivalent O sites. In the first O site, O is bonded in a 6-coordinate geometry to three equivalent Sr, one Nd, and two Fe atoms. In the second O site, O is bonded in a 6-coordinate geometry to three equivalent Sr, one Nd, and two Fe atoms. In the third O site, O is bonded in a 5-coordinate geometry to two equivalent Sr, two equivalent Nd, and two equivalent Fe atoms. In the fourth O site, O is bonded in a 6-coordinate geometry to two equivalent Sr, two equivalent Nd, and two equivalent Fe atoms. In the fifth O site, O is bonded in a 6-coordinate geometry to three equivalent Sr, one Nd, and two Fe atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li3Al(FeO3)2 by Materials Project

Li3Al(FeO3)2 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are three inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to five O2- atoms to form LiO5 trigonal bipyramids that share corners with two equivalent LiO5 trigonal bipyramids, corners with two equivalent AlO5 trigonal bipyramids, corners with four FeO5 trigonal bipyramids, an edgeedge with one AlO5 trigonal bipyramid, edges with two equivalent FeO5 trigonal bipyramids, and edges with three LiO5 trigonal bipyramids. There are a spread of Li–O bond distances ranging from 2.04–2.11 Å. In the second Li1+ site, Li1+ is bonded to five O2- atoms to form LiO5 trigonal bipyramids that share corners with two equivalent LiO5 trigonal bipyramids, corners with two equivalent AlO5 trigonal bipyramids, corners with four FeO5 trigonal bipyramids, an edgeedge with one AlO5 trigonal bipyramid, edges with two equivalent FeO5 trigonal bipyramids, and edges with three LiO5 trigonal bipyramids. There are a spread of Li–O bond distances ranging from 1.98–2.26 Å. In the third Li1+ site, Li1+ is bonded to five O2- atoms to form LiO5 trigonal bipyramids that share corners with four LiO5 trigonal bipyramids, corners with four FeO5 trigonal bipyramids, edges with two LiO5 trigonal bipyramids, edges with two FeO5 trigonal bipyramids, and edges with two equivalent AlO5 trigonal bipyramids. There are a spread of Li–O bond distances ranging from 1.97–2.13 Å. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to five O2- atoms to form FeO5 trigonal bipyramids that share corners with two equivalent AlO5 trigonal bipyramids, corners with six LiO5 trigonal bipyramids, an edgeedge with one AlO5 trigonal bipyramid, edges with two FeO5 trigonal bipyramids, and edges with three LiO5 trigonal bipyramids. There are a spread of Fe–O bond distances ranging from 1.89–2.10 Å. In the second Fe3+ site, Fe3+ is bonded to five O2- atoms to form FeO5 trigonal bipyramids that share corners with two equivalent AlO5 trigonal bipyramids, corners with six LiO5 trigonal bipyramids, an edgeedge with one AlO5 trigonal bipyramid, edges with two FeO5 trigonal bipyramids, and edges with three LiO5 trigonal bipyramids. There are a spread of Fe–O bond distances ranging from 1.92–2.10 Å. Al3+ is bonded to five O2- atoms to form AlO5 trigonal bipyramids that share corners with four LiO5 trigonal bipyramids, corners with four FeO5 trigonal bipyramids, edges with two FeO5 trigonal bipyramids, and edges with four LiO5 trigonal bipyramids. There are a spread of Al–O bond distances ranging from 1.81–2.02 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded to two Li1+, two Fe3+, and one Al3+ atom to form OLi2AlFe2 trigonal bipyramids that share corners with eight OLi2AlFe2 trigonal bipyramids and edges with six OLi3AlFe trigonal bipyramids. In the second O2- site, O2- is bonded to three Li1+, one Fe3+, and one Al3+ atom to form OLi3AlFe trigonal bipyramids that share corners with eight OLi3Fe2 trigonal bipyramids and edges with six OLi2AlFe2 trigonal bipyramids. In the third O2- site, O2- is bonded to two Li1+, two equivalent Fe3+, and one Al3+ atom to form OLi2AlFe2 trigonal bipyramids that share corners with eight OLi3Fe2 trigonal bipyramids and edges with six OLi2AlFe2 trigonal bipyramids. In the fourth O2- site, O2- is bonded to three Li1+, one Fe3+, and one Al3+ atom to form OLi3AlFe trigonal bipyramids that share corners with eight OLi3Fe2 trigonal bipyramids and edges with six OLi2AlFe2 trigonal bipyramids. In the fifth O2- site, O2- is bonded to three Li1+ and two Fe3+ atoms to form a mixture of edge and corner-sharing OLi3Fe2 trigonal bipyramids. In the sixth O2- site, O2- is bonded to two Li1+, two equivalent Fe3+, and one Al3+ atom to form OLi2AlFe2 trigonal bipyramids that share corners with eight OLi3Fe2 trigonal bipyramids and edges with six OLi2AlFe2 trigonal bipyramids.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on CsNa5(FeO3)2 by Materials Project

CsNa5(FeO3)2 crystallizes in the orthorhombic Fdd2 space group. The structure is three-dimensional. Cs1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Cs–O bond distances ranging from 3.01–3.14 Å. There are seven inequivalent Na1+ sites. In the first Na1+ site, Na1+ is bonded in a 4-coordinate geometry to four O2- atoms. There are a spread of Na–O bond distances ranging from 2.40–2.68 Å. In the second Na1+ site, Na1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Na–O bond distances ranging from 2.35–2.67 Å. In the third Na1+ site, Na1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Na–O bond distances ranging from 2.33–2.75 Å. In the fourth Na1+ site, Na1+ is bonded to five O2- atoms to form distorted NaO5 trigonal bipyramids that share corners with two FeO4 tetrahedra, an edgeedge with one NaO4 tetrahedra, and edges with two FeO4 tetrahedra. There are a spread of Na–O bond distances ranging from 2.34–2.61 Å. In the fifth Na1+ site, Na1+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Na–O bond distances ranging from 2.35–2.96 Å. In the sixth Na1+ site, Na1+ is bonded to four O2- atoms to form distorted NaO4 tetrahedra that share corners with four FeO4 tetrahedra and edges with two equivalent NaO5 trigonal bipyramids. There are two shorter (2.35 Å) and two longer (2.38 Å) Na–O bond lengths. In the seventh Na1+ site, Na1+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Na–O bond distances ranging from 2.42–2.77 Å. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to four O2- atoms to form FeO4 tetrahedra that share a cornercorner with one NaO4 tetrahedra, corners with two FeO4 tetrahedra, a cornercorner with one NaO5 trigonal bipyramid, and an edgeedge with one NaO5 trigonal bipyramid. There are a spread of Fe–O bond distances ranging from 1.86–1.96 Å. In the second Fe3+ site, Fe3+ is bonded to four O2- atoms to form FeO4 tetrahedra that share a cornercorner with one NaO4 tetrahedra, corners with two FeO4 tetrahedra, a cornercorner with one NaO5 trigonal bipyramid, and an edgeedge with one NaO5 trigonal bipyramid. There are a spread of Fe–O bond distances ranging from 1.87–1.95 Å. There are seven inequivalent O2- sites. In the first O2- site, O2- is bonded to four Na1+ and two equivalent Fe3+ atoms to form ONa4Fe2 octahedra that share corners with three equivalent ONa4Fe2 octahedra and edges with two equivalent OCsNa3Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–32°. In the second O2- site, O2- is bonded to four Na1+ and two equivalent Fe3+ atoms to form ONa4Fe2 octahedra that share corners with three equivalent ONa4Fe2 octahedra and edges with two equivalent OCsNa3Fe2 octahedra. The corner-sharing octahedra tilt angles range from 0–32°. In the third O2- site, O2- is bonded to one Cs1+, three Na1+, and two Fe3+ atoms to form distorted edge-sharing OCsNa3Fe2 octahedra. In the fourth O2- site, O2- is bonded in a 3-coordinate geometry to one Cs1+, four Na1+, and one Fe3+ atom. In the fifth O2- site, O2- is bonded in a 6-coordinate geometry to one Cs1+, four Na1+, and one Fe3+ atom. In the sixth O2- site, O2- is bonded in a 6-coordinate geometry to one Cs1+, four Na1+, and one Fe3+ atom. In the seventh O2- site, O2- is bonded in a 6-coordinate geometry to five Na1+ and one Fe3+ atom.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Sr3(FeO3)2 by Materials Project

Sr3Fe2O6 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 9-coordinate geometry to nine O2- atoms. There are a spread of Sr–O bond distances ranging from 2.48–2.82 Å. In the second Sr2+ site, Sr2+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All Sr–O bond lengths are 2.61 Å. Fe3+ is bonded to five O2- atoms to form corner-sharing FeO5 square pyramids. There is one shorter (1.91 Å) and four longer (2.01 Å) Fe–O bond length. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to five equivalent Sr2+ and one Fe3+ atom to form distorted OSr5Fe octahedra that share corners with sixteen OSr5Fe octahedra, edges with eight equivalent OSr5Fe octahedra, and faces with four equivalent OSr4Fe2 octahedra. The corner-sharing octahedra tilt angles range from 14–54°. In the second O2- site, O2- is bonded to four Sr2+ and two equivalent Fe3+ atoms to form distorted OSr4Fe2 octahedra that share corners with fourteen OSr5Fe octahedra, edges with three equivalent OSr4Fe2 octahedra, and faces with six OSr5Fe octahedra. The corner-sharing octahedra tilt angles range from 0–65°.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Li3(FeO3)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↗
DOE OSTI2020

Materials Data on Li6Mn(FeO3)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↗
DOE OSTI2020

Materials Data on Li6Mn(FeO3)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↗
DOE OSTI2020

Materials Data on Sr3Ca(FeO3)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↗
DOE OSTI2020

Materials Data on FeO3 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↗
DOE OSTI2020

Materials Data on Li3V(FeO3)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↗
DOE OSTI2020

Materials Data on Li3(FeO3)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↗
DOE OSTI2020

Materials Data on Al2(FeO3)3 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↗
DOE OSTI2020

Materials Data on Li3(FeO3)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↗
DOE OSTI2020

Materials Data on BaSr4(FeO3)5 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↗