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Materials Data on Ga(Bi3O5)4 by Materials Project

Ga(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Ga2+ is bonded to four equivalent O2- atoms to form GaO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Ga–O bond lengths are 1.89 Å. Bi+3.17+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one GaO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.59 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.17+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.17+ atoms. In the third O2- site, O2- is bonded to one Ga2+ and three equivalent Bi+3.17+ atoms to form distorted corner-sharing OGaBi3 tetrahedra.

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Materials Data on Bi3O5 by Materials Project

Bi3O5 crystallizes in the monoclinic C2/c space group. The structure is three-dimensional. there are two inequivalent Bi+3.33+ sites. In the first Bi+3.33+ site, Bi+3.33+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Bi–O bond distances ranging from 2.25–2.79 Å. In the second Bi+3.33+ site, Bi+3.33+ is bonded to six O2- atoms to form corner-sharing BiO6 octahedra. The corner-sharing octahedral tilt angles are 33°. There are a spread of Bi–O bond distances ranging from 2.17–2.35 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four Bi+3.33+ atoms to form a mixture of distorted corner and edge-sharing OBi4 tetrahedra. In the second O2- site, O2- is bonded in a 4-coordinate geometry to four Bi+3.33+ atoms. In the third O2- site, O2- is bonded in a bent 150 degrees geometry to two equivalent Bi+3.33+ atoms.

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Materials Data on Yb(Bi3O5)4 by Materials Project

Yb(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Yb2+ is bonded in a distorted body-centered cubic geometry to eight O2- atoms. There are four shorter (2.31 Å) and four longer (2.91 Å) Yb–O bond lengths. Bi+3.17+ is bonded to five O2- atoms to form a mixture of distorted corner and edge-sharing BiO5 square pyramids. There are a spread of Bi–O bond distances ranging from 2.11–2.52 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to one Yb2+ and three equivalent Bi+3.17+ atoms to form a mixture of distorted corner and edge-sharing OYbBi3 trigonal pyramids. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.17+ atoms. In the third O2- site, O2- is bonded to one Yb2+ and three equivalent Bi+3.17+ atoms to form a mixture of corner and edge-sharing OYbBi3 tetrahedra.

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Materials Data on Li(Bi3O5)4 by Materials Project

Li(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Li1+ is bonded to four equivalent O2- atoms to form LiO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Li–O bond lengths are 2.10 Å. Bi+3.25+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one LiO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.10–2.53 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.25+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.25+ atoms. In the third O2- site, O2- is bonded to one Li1+ and three equivalent Bi+3.25+ atoms to form corner-sharing OLiBi3 tetrahedra.

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Materials Data on Ho(Bi3O5)4 by Materials Project

Ho(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Ho3+ is bonded to four equivalent O2- atoms to form HoO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Ho–O bond lengths are 2.17 Å. Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one HoO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.10–2.55 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.08+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.08+ atoms. In the third O2- site, O2- is bonded to one Ho3+ and three equivalent Bi+3.08+ atoms to form corner-sharing OHoBi3 tetrahedra.

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Materials Data on Y(Bi3O5)4 by Materials Project

Y(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Y3+ is bonded to four equivalent O2- atoms to form YO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Y–O bond lengths are 2.19 Å. Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one YO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.54 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.08+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.08+ atoms. In the third O2- site, O2- is bonded to one Y3+ and three equivalent Bi+3.08+ atoms to form corner-sharing OYBi3 tetrahedra.

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Materials Data on Be(Bi3O5)4 by Materials Project

Be(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Be2+ is bonded to four equivalent O2- atoms to form BeO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Be–O bond lengths are 1.71 Å. Bi+3.17+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one BeO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.56 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to one Be2+ and three equivalent Bi+3.17+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.17+ atoms. In the third O2- site, O2- is bonded in a trigonal non-coplanar geometry to three equivalent Bi+3.17+ atoms.

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Materials Data on Er(Bi3O5)4 by Materials Project

Er(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Er3+ is bonded to four equivalent O2- atoms to form ErO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Er–O bond lengths are 2.15 Å. Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one ErO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.55 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to one Er3+ and three equivalent Bi+3.08+ atoms to form corner-sharing OErBi3 tetrahedra. In the second O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.08+ atoms. In the third O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.08+ atoms.

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Materials Data on Dy(Bi3O5)4 by Materials Project

Dy(Bi3O5)4 crystallizes in the orthorhombic I222 space group. The structure is three-dimensional. Dy3+ is bonded to four equivalent O2- atoms to form DyO4 tetrahedra that share corners with twelve BiO5 square pyramids. All Dy–O bond lengths are 2.20 Å. There are three inequivalent Bi+3.08+ sites. In the first Bi+3.08+ site, Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight BiO5 square pyramids, a cornercorner with one DyO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.54 Å. In the second Bi+3.08+ site, Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight BiO5 square pyramids, a cornercorner with one DyO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.55 Å. In the third Bi+3.08+ site, Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight BiO5 square pyramids, a cornercorner with one DyO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.54 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Bi+3.08+ atoms. In the second O2- site, O2- is bonded in a trigonal planar geometry to three Bi+3.08+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Bi+3.08+ atoms. In the fourth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three Bi+3.08+ atoms. In the fifth O2- site, O2- is bonded to one Dy3+ and three Bi+3.08+ atoms to form corner-sharing ODyBi3 tetrahedra.

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Materials Data on Al(Bi3O5)4 by Materials Project

Al(Bi3O5)4 crystallizes in the cubic I23 space group. The structure is three-dimensional. Al3+ is bonded to four equivalent O2- atoms to form AlO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Al–O bond lengths are 1.80 Å. Bi+3.08+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one AlO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.61 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.08+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Al3+ and three equivalent Bi+3.08+ atoms. In the third O2- site, O2- is bonded in a 3-coordinate geometry to three equivalent Bi+3.08+ atoms.

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Materials Data on Ge(Bi3O5)4 by Materials Project

Bi12GeO20 crystallizes in the cubic I23 space group. The structure is three-dimensional. Ge4+ is bonded in a tetrahedral geometry to four equivalent O2- atoms. All Ge–O bond lengths are 1.80 Å. Bi3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Bi–O bond distances ranging from 2.11–2.66 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the second O2- site, O2- is bonded to one Ge4+ and three equivalent Bi3+ atoms to form distorted corner-sharing OGeBi3 tetrahedra. In the third O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi3+ atoms.

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Materials Data on Si(Bi3O5)4 by Materials Project

Bi12SiO20 crystallizes in the cubic I23 space group. The structure is three-dimensional. Si4+ is bonded in a tetrahedral geometry to four equivalent O2- atoms. All Si–O bond lengths are 1.67 Å. Bi3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Bi–O bond distances ranging from 2.11–2.68 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 3-coordinate geometry to three equivalent Bi3+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Si4+ and three equivalent Bi3+ atoms. In the third O2- site, O2- is bonded in a trigonal non-coplanar geometry to three equivalent Bi3+ atoms.

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Materials Data on Ti(Bi3O5)4 by Materials Project

Bi12TiO20 crystallizes in the cubic I23 space group. The structure is three-dimensional. Ti4+ is bonded in a tetrahedral geometry to four equivalent O2- atoms. All Ti–O bond lengths are 1.85 Å. Bi3+ is bonded in a 5-coordinate geometry to five O2- atoms. There are a spread of Bi–O bond distances ranging from 2.11–2.65 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi3+ atoms. In the second O2- site, O2- is bonded in a distorted single-bond geometry to one Ti4+ and three equivalent Bi3+ atoms. In the third O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi3+ atoms.

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Materials Data on Zn(Bi3O5)4 by Materials Project

ZnBi12O20 crystallizes in the cubic I23 space group. The structure is three-dimensional. Zn2+ is bonded to four equivalent O2- atoms to form ZnO4 tetrahedra that share corners with twelve equivalent BiO5 square pyramids. All Zn–O bond lengths are 2.03 Å. Bi+3.17+ is bonded to five O2- atoms to form distorted BiO5 square pyramids that share corners with eight equivalent BiO5 square pyramids, a cornercorner with one ZnO4 tetrahedra, and an edgeedge with one BiO5 square pyramid. There are a spread of Bi–O bond distances ranging from 2.11–2.56 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to one Zn2+ and three equivalent Bi+3.17+ atoms to form corner-sharing OZnBi3 tetrahedra. In the second O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Bi+3.17+ atoms. In the third O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to three equivalent Bi+3.17+ atoms.

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Materials Data on Co(Bi3O5)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

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Materials Data on Mn(Bi3O5)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

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