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Materials Data on Ba4CaCr4Cu2F28 by Materials Project

Ba4CaCr4Cu2F28 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are four inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten F1- atoms. There are a spread of Ba–F bond distances ranging from 2.70–3.02 Å. In the second Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten F1- atoms. There are a spread of Ba–F bond distances ranging from 2.62–3.00 Å. In the third Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten F1- atoms. There are a spread of Ba–F bond distances ranging from 2.61–3.02 Å. In the fourth Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to ten F1- atoms. There are a spread of Ba–F bond distances ranging from 2.72–3.00 Å. Ca2+ is bonded in a 8-coordinate geometry to eight F1- atoms. There are a spread of Ca–F bond distances ranging from 2.32–2.63 Å. There are four inequivalent Cr+3.75+ sites. In the first Cr+3.75+ site, Cr+3.75+ is bonded to six F1- atoms to form CrF6 octahedra that share corners with two equivalent CuF6 octahedra. The corner-sharing octahedra tilt angles range from 46–61°. There are a spread of Cr–F bond distances ranging from 1.81–1.96 Å. In the second Cr+3.75+ site, Cr+3.75+ is bonded to six F1- atoms to form CrF6 octahedra that share corners with two equivalent CuF6 octahedra. The corner-sharing octahedra tilt angles range from 46–61°. There are a spread of Cr–F bond distances ranging from 1.93–1.97 Å. In the third Cr+3.75+ site, Cr+3.75+ is bonded to six F1- atoms to form CrF6 octahedra that share corners with two equivalent CuF6 octahedra. The corner-sharing octahedra tilt angles range from 46–61°. There are a spread of Cr–F bond distances ranging from 1.92–1.97 Å. In the fourth Cr+3.75+ site, Cr+3.75+ is bonded to six F1- atoms to form CrF6 octahedra that share corners with two equivalent CuF6 octahedra. The corner-sharing octahedra tilt angles range from 46–60°. There are a spread of Cr–F bond distances ranging from 1.80–1.96 Å. There are two inequivalent Cu+1.50+ sites. In the first Cu+1.50+ site, Cu+1.50+ is bonded to six F1- atoms to form distorted CuF6 octahedra that share corners with four CrF6 octahedra. The corner-sharing octahedra tilt angles range from 46–61°. There are a spread of Cu–F bond distances ranging from 1.84–2.50 Å. In the second Cu+1.50+ site, Cu+1.50+ is bonded to six F1- atoms to form distorted CuF6 octahedra that share corners with four CrF6 octahedra. The corner-sharing octahedra tilt angles range from 46–61°. There are a spread of Cu–F bond distances ranging from 1.84–2.52 Å. There are twenty-eight inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted single-bond geometry to two equivalent Ba2+ and one Cr+3.75+ atom. In the second F1- site, F1- is bonded in a 1-coordinate geometry to two equivalent Ba2+ and one Cr+3.75+ atom. In the third F1- site, F1- is bonded in a 3-coordinate geometry to one Ba2+, one Ca2+, and one Cr+3.75+ atom. In the fourth F1- site, F1- is bonded in a 3-coordinate geometry to one Ba2+, one Ca2+, and one Cr+3.75+ atom. In the fifth F1- site, F1- is bonded in a 2-coordinate geometry to one Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the sixth F1- site, F1- is bonded in a 2-coordinate geometry to one Ba2+, one Ca2+, and one Cr+3.75+ atom. In the seventh F1- site, F1- is bonded in a 2-coordinate geometry to one Ba2+, one Ca2+, and one Cr+3.75+ atom. In the eighth F1- site, F1- is bonded in a 1-coordinate geometry to two equivalent Ba2+ and one Cr+3.75+ atom. In the ninth F1- site, F1- is bonded in a distorted single-bond geometry to one Ba2+ and one Cr+3.75+ atom. In the tenth F1- site, F1- is bonded in a 1-coordinate geometry to two Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the eleventh F1- site, F1- is bonded in a 1-coordinate geometry to two Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the twelfth F1- site, F1- is bonded in a 3-coordinate geometry to one Ba2+, one Ca2+, and one Cu+1.50+ atom. In the thirteenth F1- site, F1- is bonded in a distorted single-bond geometry to one Ba2+ and one Cr+3.75+ atom. In the fourteenth F1- site, F1- is bonded in a single-bond geometry to one Ba2+ and one Cr+3.75+ atom. In the fifteenth F1- site, F1- is bonded in a distorted single-bond geometry to two Ba2+ and one Cr+3.75+ atom. In the sixteenth F1- site, F1- is bonded in a distorted single-bond geometry to two equivalent Ba2+ and one Cr+3.75+ atom. In the seventeenth F1- site, F1- is bonded in a 2-coordinate geometry to one Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the eighteenth F1- site, F1- is bonded in a 1-coordinate geometry to two Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the nineteenth F1- site, F1- is bonded in a distorted single-bond geometry to two Ba2+ and one Cr+3.75+ atom. In the twentieth F1- site, F1- is bonded in a distorted single-bond geometry to two Ba2+, one Ca2+, and one Cr+3.75+ atom. In the twenty-first F1- site, F1- is bonded in a 3-coordinate geometry to one Ba2+, one Ca2+, and one Cu+1.50+ atom. In the twenty-second F1- site, F1- is bonded in a distorted bent 120 degrees geometry to one Ba2+ and one Cu+1.50+ atom. In the twenty-third F1- site, F1- is bonded in a distorted single-bond geometry to two Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the twenty-fourth F1- site, F1- is bonded in a 2-coordinate geometry to one Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the twenty-fifth F1- site, F1- is bonded in a 2-coordinate geometry to one Ba2+, one Cr+3.75+, and one Cu+1.50+ atom. In the twenty-sixth F1- site, F1- is bonded in a 1-coordinate geometry to two Ba2+, one Ca2+, and one Cr+3.75+ atom. In the twenty-seventh F1- site, F1- is bonded in a single-bond geometry to one Ba2+ and one Cr+3.75+ atom. In the twenty-eighth F1- site, F1- is bonded in a distorted bent 120 degrees geometry to one Ba2+ and one Cu+1.50+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Ba2CaCr2CuF14 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↗