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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
Bi26Mo10O69 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are five inequivalent Mo sites. In the first Mo site, Mo is bonded in a tetrahedral geometry to four O atoms. There are a spread of Mo–O bond distances ranging from 1.79–1.82 Å. In the second Mo site, Mo is bonded to five O atoms to form corner-sharing MoO5 trigonal bipyramids. There are a spread of Mo–O bond distances ranging from 1.83–1.98 Å. In the third Mo site, Mo is bonded to four O atoms to form MoO4 tetrahedra that share a cornercorner with one BiO6 octahedra. The corner-sharing octahedral tilt angles are 51°. There are a spread of Mo–O bond distances ranging from 1.77–1.86 Å. In the fourth Mo site, Mo is bonded to four O atoms to form MoO4 tetrahedra that share corners with two equivalent BiO6 octahedra. The corner-sharing octahedra tilt angles range from 49–59°. There are a spread of Mo–O bond distances ranging from 1.78–1.83 Å. In the fifth Mo site, Mo is bonded in a tetrahedral geometry to four O atoms. There are a spread of Mo–O bond distances ranging from 1.78–1.85 Å. There are fourteen inequivalent Bi sites. In the first Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.18–2.61 Å. In the second Bi site, Bi is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Bi–O bond distances ranging from 2.18–2.73 Å. In the third Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.22–2.70 Å. In the fourth Bi site, Bi is bonded in a rectangular see-saw-like geometry to four O atoms. There are a spread of Bi–O bond distances ranging from 2.14–2.37 Å. In the fifth Bi site, Bi is bonded in a 6-coordinate geometry to six O atoms. There are a spread of Bi–O bond distances ranging from 2.14–2.70 Å. In the sixth Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.15–2.56 Å. In the seventh Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.23–2.65 Å. In the eighth Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.20–2.43 Å. In the ninth Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.16–2.74 Å. In the tenth Bi site, Bi is bonded in a distorted rectangular see-saw-like geometry to four O atoms. There are a spread of Bi–O bond distances ranging from 2.15–2.64 Å. In the eleventh Bi site, Bi is bonded in a 5-coordinate geometry to five O atoms. There are a spread of Bi–O bond distances ranging from 2.17–2.74 Å. In the twelfth Bi site, Bi is bonded in a 4-coordinate geometry to four O atoms. There are a spread of Bi–O bond distances ranging from 2.14–2.66 Å. In the thirteenth Bi site, Bi is bonded in a square co-planar geometry to four O atoms. There are two shorter (2.30 Å) and two longer (2.35 Å) Bi–O bond lengths. In the fourteenth Bi site, Bi is bonded to six O atoms to form BiO6 octahedra that share corners with six MoO4 tetrahedra. There are a spread of Bi–O bond distances ranging from 2.34–2.44 Å. There are thirty-five inequivalent O sites. In the first O site, O is bonded to four Bi atoms to form distorted edge-sharing OBi4 tetrahedra. In the second O site, O is bonded to four Bi atoms to form edge-sharing OBi4 tetrahedra. In the third O site, O is bonded in a trigonal non-coplanar geometry to three Bi atoms. In the fourth O site, O is bonded in a trigonal planar geometry to three Bi atoms. In the fifth O site, O is bonded in a distorted trigonal non-coplanar geometry to three Bi atoms. In the sixth O site, O is bonded in a distorted trigonal non-coplanar geometry to three Bi atoms. In the seventh O site, O is bonded in a distorted trigonal non-coplanar geometry to three Bi atoms. In the eighth O site, O is bonded in a trigonal non-coplanar geometry to three Bi atoms. In the ninth O site, O is bonded in a distorted trigonal planar geometry to three Bi atoms. In the tenth O site, O is bonded in a trigonal non-coplanar geometry to three Bi atoms. In the eleventh O site, O is bonded in a trigonal planar geometry to three Bi atoms. In the twelfth O site, O is bonded in a trigonal non-coplanar geometry to three Bi atoms. In the thirteenth O site, O is bonded in a trigonal planar geometry to three Bi atoms. In the fourteenth O site, O is bonded in a trigonal non-coplanar geometry to three Bi atoms. In the fifteenth O site, O is bonded in a single-bond geometry to one Mo atom. In the sixteenth O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the seventeenth O site, O is bonded in a bent 150 degrees geometry to one Mo and one Bi atom. In the eighteenth O site, O is bonded in a 1-coordinate geometry to one Mo and two Bi atoms. In the nineteenth O site, O is bonded in a distorted bent 120 degrees geometry to one Mo and one Bi atom. In the twentieth O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the twenty-first O site, O is bonded in a bent 120 degrees geometry to one Mo and one Bi atom. In the twenty-second O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the twenty-third O site, O is bonded in a distorted bent 120 degrees geometry to one Mo and one Bi atom. In the twenty-fourth O site, O is bonded in a distorted bent 150 degrees geometry to one Mo and one Bi atom. In the twenty-fifth O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the twenty-sixth O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the twenty-seventh O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the twenty-eighth O site, O is bonded in a bent 120 degrees geometry to one Mo and one Bi atom. In the twenty-ninth O site, O is bonded in a distorted bent 120 degrees geometry to one Mo and one Bi atom. In the thirtieth O site, O is bonded in a linear geometry to one Mo and one Bi atom. In the thirty-first O site, O is bonded in a distorted single-bond geometry to one Mo and one Bi atom. In the thirty-second O site, O is bonded in a distorted bent 150 degrees geometry to one Mo and one Bi atom. In the thirty-third O site, O is bonded in a 1-coordinate geometry to one Mo and two Bi atoms. In the thirty-fourth O site, O is bonded in a single-bond geometry to one Mo atom. In the thirty-fifth O site, O is bonded in a linear geometry to two equivalent Mo atoms.
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