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Materials Data on CaSn2F6 by Materials Project

CaSn2F6 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Ca2+ is bonded in a 8-coordinate geometry to eight F1- atoms. There are a spread of Ca–F bond distances ranging from 2.33–2.49 Å. There are two inequivalent Sn2+ sites. In the first Sn2+ site, Sn2+ is bonded in a 4-coordinate geometry to four F1- atoms. There are a spread of Sn–F bond distances ranging from 2.11–2.59 Å. In the second Sn2+ site, Sn2+ is bonded in a 4-coordinate geometry to five F1- atoms. There are a spread of Sn–F bond distances ranging from 2.09–2.71 Å. There are six inequivalent F1- sites. In the first F1- site, F1- is bonded in a 1-coordinate geometry to three Sn2+ atoms. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Ca2+ and one Sn2+ atom. In the third F1- site, F1- is bonded in a distorted bent 150 degrees geometry to one Ca2+ and one Sn2+ atom. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to two equivalent Ca2+ and one Sn2+ atom. In the fifth F1- site, F1- is bonded in a 3-coordinate geometry to one Ca2+ and two equivalent Sn2+ atoms. In the sixth F1- site, F1- is bonded in a 3-coordinate geometry to two equivalent Ca2+ and one Sn2+ atom.

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Materials Data on CaSnF6 by Materials Project

CaSnF6 crystallizes in the trigonal R-3 space group. The structure is three-dimensional. Ca2+ is bonded to six equivalent F1- atoms to form CaF6 octahedra that share corners with six equivalent SnF6 octahedra. The corner-sharing octahedral tilt angles are 23°. All Ca–F bond lengths are 2.27 Å. Sn4+ is bonded to six equivalent F1- atoms to form SnF6 octahedra that share corners with six equivalent CaF6 octahedra. The corner-sharing octahedral tilt angles are 23°. All Sn–F bond lengths are 2.00 Å. F1- is bonded in a bent 150 degrees geometry to one Ca2+ and one Sn4+ atom.

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Materials Data on CaSnF6 by Materials Project

CaSnF6 is High-temperature superconductor-derived structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ca2+ is bonded to six equivalent F1- atoms to form CaF6 octahedra that share corners with six equivalent SnF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ca–F bond lengths are 2.27 Å. Sn4+ is bonded to six equivalent F1- atoms to form SnF6 octahedra that share corners with six equivalent CaF6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Sn–F bond lengths are 2.00 Å. F1- is bonded in a linear geometry to one Ca2+ and one Sn4+ atom.

36 MATERIALS SCIENCE↗

Materials Data on CaSnF5 by Materials Project

CaSnF5 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. Ca2+ is bonded to seven F1- atoms to form distorted CaF7 pentagonal bipyramids that share corners with four equivalent SnF6 octahedra, edges with two equivalent SnF6 octahedra, and edges with two equivalent CaF7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 13–48°. There are a spread of Ca–F bond distances ranging from 2.23–2.60 Å. Sn3+ is bonded to six F1- atoms to form SnF6 octahedra that share corners with two equivalent SnF6 octahedra, corners with four equivalent CaF7 pentagonal bipyramids, and edges with two equivalent CaF7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 35°. There are a spread of Sn–F bond distances ranging from 2.11–2.22 Å. There are five inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Ca2+ and one Sn3+ atom. In the second F1- site, F1- is bonded in a distorted trigonal planar geometry to two equivalent Ca2+ and one Sn3+ atom. In the third F1- site, F1- is bonded in a bent 150 degrees geometry to one Ca2+ and one Sn3+ atom. In the fourth F1- site, F1- is bonded in a linear geometry to one Ca2+ and one Sn3+ atom. In the fifth F1- site, F1- is bonded in a 3-coordinate geometry to one Ca2+ and two equivalent Sn3+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on CaSnF4 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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