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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
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
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
NaFe5O8 is Spinel-like structured and crystallizes in the cubic P4_332 space group. The structure is three-dimensional. Na1+ is bonded to six equivalent O2- atoms to form NaO6 octahedra that share corners with six equivalent FeO4 tetrahedra and edges with six equivalent FeO6 octahedra. All Na–O bond lengths are 2.30 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 corners with three equivalent NaO6 octahedra and corners with nine equivalent FeO6 octahedra. The corner-sharing octahedra tilt angles range from 51–63°. There is three shorter (1.93 Å) and one longer (1.99 Å) Fe–O bond length. In the second Fe3+ site, Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six equivalent FeO4 tetrahedra, edges with two equivalent NaO6 octahedra, and edges with four equivalent FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 2.02–2.09 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to one Na1+ and three Fe3+ atoms. In the second O2- site, O2- is bonded to four Fe3+ atoms to form distorted corner-sharing OFe4 trigonal pyramids.
Na(FeO2)2 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Na sites. In the first Na site, Na is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Na–O bond distances ranging from 2.42–2.57 Å. In the second Na site, Na is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Na–O bond distances ranging from 2.41–2.57 Å. In the third Na site, Na is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Na–O bond distances ranging from 2.40–2.55 Å. In the fourth Na site, Na is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Na–O bond distances ranging from 2.45–2.56 Å. There are eight inequivalent Fe sites. In the first Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.99–2.10 Å. In the second Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 2.00–2.09 Å. In the third Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.99–2.07 Å. In the fourth Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.99–2.08 Å. In the fifth Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.96–2.01 Å. In the sixth Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are five shorter (2.03 Å) and one longer (2.04 Å) Fe–O bond lengths. In the seventh Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are a spread of Fe–O bond distances ranging from 1.97–1.99 Å. In the eighth Fe site, Fe is bonded to six O atoms to form edge-sharing FeO6 octahedra. There are three shorter (2.03 Å) and three longer (2.04 Å) Fe–O bond lengths. There are sixteen inequivalent O sites. In the first O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the second O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the third O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the fourth O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the fifth O site, O is bonded to one Na and three Fe atoms to form distorted ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the sixth O site, O is bonded to one Na and three Fe atoms to form distorted ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the seventh O site, O is bonded to one Na and three Fe atoms to form ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the eighth O site, O is bonded to one Na and three Fe atoms to form ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the ninth O site, O is bonded to one Na and three Fe atoms to form ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the tenth O site, O is bonded to one Na and three Fe atoms to form ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the eleventh O site, O is bonded to one Na and three Fe atoms to form ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the twelfth O site, O is bonded to one Na and three Fe atoms to form distorted ONaFe3 trigonal pyramids that share corners with four ONa2Fe3 trigonal bipyramids, corners with six ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and an edgeedge with one ONaFe3 trigonal pyramid. In the thirteenth O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the fourteenth O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the fifteenth O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids. In the sixteenth O site, O is bonded to two Na and three Fe atoms to form ONa2Fe3 trigonal bipyramids that share corners with five ONa2Fe3 trigonal bipyramids, corners with four ONaFe3 trigonal pyramids, edges with four ONa2Fe3 trigonal bipyramids, and edges with four ONaFe3 trigonal pyramids.
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
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
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
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
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
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
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
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
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
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
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
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
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