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Materials Data on Ca4TiN4 by Materials Project

Ca4TiN4 crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are four inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded to five N3- atoms to form CaN5 square pyramids that share corners with three equivalent CaN5 square pyramids, a cornercorner with one TiN4 tetrahedra, corners with two equivalent CaN4 trigonal pyramids, edges with five CaN5 square pyramids, and edges with two equivalent TiN4 tetrahedra. There are a spread of Ca–N bond distances ranging from 2.44–2.59 Å. In the second Ca2+ site, Ca2+ is bonded in a 5-coordinate geometry to five N3- atoms. There are a spread of Ca–N bond distances ranging from 2.42–2.86 Å. In the third Ca2+ site, Ca2+ is bonded to four N3- atoms to form distorted CaN4 trigonal pyramids that share corners with four CaN5 square pyramids, corners with four equivalent TiN4 tetrahedra, and edges with two equivalent CaN4 trigonal pyramids. There are a spread of Ca–N bond distances ranging from 2.40–2.49 Å. In the fourth Ca2+ site, Ca2+ is bonded to five N3- atoms to form CaN5 square pyramids that share corners with three equivalent CaN5 square pyramids, corners with three equivalent TiN4 tetrahedra, corners with two equivalent CaN4 trigonal pyramids, edges with five CaN5 square pyramids, and an edgeedge with one TiN4 tetrahedra. There are a spread of Ca–N bond distances ranging from 2.41–2.50 Å. Ti4+ is bonded to four N3- atoms to form TiN4 tetrahedra that share corners with four CaN5 square pyramids, corners with four equivalent CaN4 trigonal pyramids, and edges with three CaN5 square pyramids. There are a spread of Ti–N bond distances ranging from 1.94–1.98 Å. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded to five Ca2+ and one Ti4+ atom to form a mixture of corner and edge-sharing NCa5Ti octahedra. The corner-sharing octahedra tilt angles range from 6–20°. In the second N3- site, N3- is bonded to five Ca2+ and one Ti4+ atom to form a mixture of distorted corner and edge-sharing NCa5Ti octahedra. The corner-sharing octahedra tilt angles range from 6–20°. In the third N3- site, N3- is bonded to five Ca2+ and one Ti4+ atom to form a mixture of corner and edge-sharing NCa5Ti octahedra. The corner-sharing octahedra tilt angles range from 11–16°. In the fourth N3- site, N3- is bonded in a 5-coordinate geometry to four Ca2+ and one Ti4+ atom.

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Materials Data on Ca2TiN2 by Materials Project

Ca2TiN2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded to five N3- atoms to form a mixture of edge and corner-sharing CaN5 square pyramids. There are a spread of Ca–N bond distances ranging from 2.52–2.69 Å. In the second Ca2+ site, Ca2+ is bonded in a rectangular see-saw-like geometry to four N3- atoms. There are a spread of Ca–N bond distances ranging from 2.36–2.60 Å. Ti2+ is bonded in a T-shaped geometry to three N3- atoms. There are two shorter (1.92 Å) and one longer (2.11 Å) Ti–N bond lengths. There are two inequivalent N3- sites. In the first N3- site, N3- is bonded to five Ca2+ and one Ti2+ atom to form a mixture of edge and corner-sharing NCa5Ti octahedra. The corner-sharing octahedra tilt angles range from 8–18°. In the second N3- site, N3- is bonded to four Ca2+ and two equivalent Ti2+ atoms to form a mixture of edge and corner-sharing NCa4Ti2 octahedra. The corner-sharing octahedra tilt angles range from 8–18°.

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Materials Data on Ca3(TiN2)2 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 Ca3TiN3 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 Ca3(TiN2)2 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 Ca3Ti3N5 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 Ca7TiN6 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↗

Materials Data on Ca11(TiN5)2 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↗

Materials Data on CaTiN2 by Materials Project

CaTiN2 crystallizes in the orthorhombic Pbca space group. The structure is three-dimensional. there are two inequivalent Ca2+ sites. In the first Ca2+ site, Ca2+ is bonded to six N3- atoms to form CaN6 octahedra that share corners with four equivalent CaN6 octahedra, corners with six TiN4 tetrahedra, edges with four CaN6 octahedra, and edges with three TiN4 tetrahedra. The corner-sharing octahedra tilt angles range from 20–22°. There are a spread of Ca–N bond distances ranging from 2.42–2.65 Å. In the second Ca2+ site, Ca2+ is bonded to six N3- atoms to form CaN6 octahedra that share corners with four equivalent CaN6 octahedra, corners with six TiN4 tetrahedra, edges with four CaN6 octahedra, and edges with three TiN4 tetrahedra. The corner-sharing octahedra tilt angles range from 20–23°. There are a spread of Ca–N bond distances ranging from 2.43–2.64 Å. There are two inequivalent Ti4+ sites. In the first Ti4+ site, Ti4+ is bonded to four N3- atoms to form TiN4 tetrahedra that share corners with six CaN6 octahedra, corners with four TiN4 tetrahedra, and edges with three CaN6 octahedra. The corner-sharing octahedra tilt angles range from 29–81°. There are a spread of Ti–N bond distances ranging from 1.91–2.02 Å. In the second Ti4+ site, Ti4+ is bonded to four N3- atoms to form TiN4 tetrahedra that share corners with six CaN6 octahedra, corners with four TiN4 tetrahedra, and edges with three CaN6 octahedra. The corner-sharing octahedra tilt angles range from 29–80°. There are a spread of Ti–N bond distances ranging from 1.91–2.02 Å. There are four inequivalent N3- sites. In the first N3- site, N3- is bonded to three Ca2+ and two equivalent Ti4+ atoms to form a mixture of distorted edge and corner-sharing NCa3Ti2 trigonal bipyramids. In the second N3- site, N3- is bonded in a 5-coordinate geometry to three Ca2+ and two equivalent Ti4+ atoms. In the third N3- site, N3- is bonded to three equivalent Ca2+ and two Ti4+ atoms to form a mixture of distorted edge and corner-sharing NCa3Ti2 trigonal bipyramids. In the fourth N3- site, N3- is bonded in a 5-coordinate geometry to three equivalent Ca2+ and two Ti4+ atoms.

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Materials Data on Ca5(TiN3)2 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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