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Materials Data on Cr3(MoC2)2 by Materials Project

Cr3(MoC2)2 is MAX Phase-like structured and crystallizes in the trigonal R3m space group. The structure is two-dimensional and consists of three Cr3(MoC2)2 sheets oriented in the (0, 0, 1) direction. there are two inequivalent Mo4+ sites. In the first Mo4+ site, Mo4+ is bonded to six C4- atoms to form MoC6 octahedra that share corners with three equivalent CrC6 octahedra, edges with three equivalent CrC6 octahedra, and edges with six equivalent MoC6 octahedra. The corner-sharing octahedral tilt angles are 5°. There are three shorter (2.15 Å) and three longer (2.20 Å) Mo–C bond lengths. In the second Mo4+ site, Mo4+ is bonded in a distorted T-shaped geometry to three equivalent C4- atoms. All Mo–C bond lengths are 2.10 Å. There are three inequivalent Cr+2.67+ sites. In the first Cr+2.67+ site, Cr+2.67+ is bonded in a trigonal non-coplanar geometry to three equivalent C4- atoms. All Cr–C bond lengths are 1.93 Å. In the second Cr+2.67+ site, Cr+2.67+ is bonded to six C4- atoms to form a mixture of corner and edge-sharing CrC6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (2.06 Å) and three longer (2.10 Å) Cr–C bond lengths. In the third Cr+2.67+ site, Cr+2.67+ is bonded to six C4- atoms to form CrC6 octahedra that share corners with three equivalent MoC6 octahedra, corners with three equivalent CrC6 octahedra, edges with three equivalent MoC6 octahedra, and edges with nine CrC6 octahedra. The corner-sharing octahedra tilt angles range from 2–5°. There are three shorter (2.02 Å) and three longer (2.11 Å) Cr–C bond lengths. There are four inequivalent C4- sites. In the first C4- site, C4- is bonded to six Cr+2.67+ atoms to form a mixture of corner and edge-sharing CCr6 octahedra. The corner-sharing octahedral tilt angles are 2°. In the second C4- site, C4- is bonded to six Cr+2.67+ atoms to form CCr6 octahedra that share corners with six CCr3Mo3 octahedra and edges with twelve CCr6 octahedra. The corner-sharing octahedra tilt angles range from 2–3°. In the third C4- site, C4- is bonded to three equivalent Mo4+ and three equivalent Cr+2.67+ atoms to form a mixture of corner and edge-sharing CCr3Mo3 octahedra. The corner-sharing octahedra tilt angles range from 2–3°. In the fourth C4- site, C4- is bonded to six Mo4+ atoms to form a mixture of corner and edge-sharing CMo6 octahedra. The corner-sharing octahedral tilt angles are 2°.

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Materials Data on Cr3(P2O7)2 by Materials Project

Cr3(P2O7)2 crystallizes in the triclinic P-1 space group. The structure is two-dimensional and consists of one Cr3(P2O7)2 sheet oriented in the (0, 0, 1) direction. there are three inequivalent Cr+2.67+ sites. In the first Cr+2.67+ site, Cr+2.67+ is bonded to six O2- atoms to form CrO6 octahedra that share corners with six PO4 tetrahedra. There are a spread of Cr–O bond distances ranging from 1.93–2.23 Å. In the second Cr+2.67+ site, Cr+2.67+ is bonded to five O2- atoms to form CrO5 trigonal bipyramids that share corners with five PO4 tetrahedra. There are a spread of Cr–O bond distances ranging from 2.02–2.24 Å. In the third Cr+2.67+ site, Cr+2.67+ is bonded in a 6-coordinate geometry to six O2- atoms. There are a spread of Cr–O bond distances ranging from 2.03–2.62 Å. There are four inequivalent P5+ sites. In the first P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent CrO6 octahedra, a cornercorner with one PO4 tetrahedra, and a cornercorner with one CrO5 trigonal bipyramid. The corner-sharing octahedra tilt angles range from 38–50°. There are a spread of P–O bond distances ranging from 1.51–1.57 Å. In the second P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent CrO6 octahedra and a cornercorner with one PO4 tetrahedra. The corner-sharing octahedra tilt angles range from 37–42°. There are a spread of P–O bond distances ranging from 1.50–1.66 Å. In the third P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share a cornercorner with one PO4 tetrahedra and corners with three equivalent CrO5 trigonal bipyramids. There are a spread of P–O bond distances ranging from 1.52–1.63 Å. In the fourth P5+ site, P5+ is bonded to four O2- atoms to form PO4 tetrahedra that share corners with two equivalent CrO6 octahedra, a cornercorner with one PO4 tetrahedra, and a cornercorner with one CrO5 trigonal bipyramid. The corner-sharing octahedra tilt angles range from 23–46°. There are a spread of P–O bond distances ranging from 1.49–1.62 Å. There are fourteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 120 degrees geometry to two P5+ atoms. In the second O2- site, O2- is bonded in a 3-coordinate geometry to two Cr+2.67+ and one P5+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to two Cr+2.67+ and one P5+ atom. In the fourth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cr+2.67+ and one P5+ atom. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cr+2.67+ and one P5+ atom. In the sixth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cr+2.67+ and one P5+ atom. In the seventh O2- site, O2- is bonded in a single-bond geometry to one P5+ atom. In the eighth O2- site, O2- is bonded in a distorted trigonal planar geometry to two Cr+2.67+ and one P5+ atom. In the ninth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr+2.67+ and one P5+ atom. In the tenth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr+2.67+ and one P5+ atom. In the eleventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr+2.67+ and one P5+ atom. In the twelfth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr+2.67+ and one P5+ atom. In the thirteenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr+2.67+ and one P5+ atom. In the fourteenth O2- site, O2- is bonded in a bent 150 degrees geometry to two P5+ atoms.

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Materials Data on Cr3(W10C3)2 by Materials Project

Cr3(W10C3)2 crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. there are two inequivalent W sites. In the first W site, W is bonded in a 3-coordinate geometry to one Cr and two equivalent C atoms. The W–Cr bond length is 2.75 Å. Both W–C bond lengths are 2.33 Å. In the second W site, W is bonded to one Cr and three equivalent C atoms to form a mixture of edge and corner-sharing WCrC3 tetrahedra. The W–Cr bond length is 2.63 Å. All W–C bond lengths are 2.29 Å. There are two inequivalent Cr sites. In the first Cr site, Cr is bonded in a cuboctahedral geometry to twelve equivalent W atoms. In the second Cr site, Cr is bonded in a distorted tetrahedral geometry to four equivalent W atoms. C is bonded in a 8-coordinate geometry to eight W atoms.

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Materials Data on Cr3(TeSe)2 by Materials Project

Cr3(TeSe)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Cr+2.67+ sites. In the first Cr+2.67+ site, Cr+2.67+ is bonded to four equivalent Te2- and two equivalent Se2- atoms to form CrTe4Se2 octahedra that share corners with twelve equivalent CrTe3Se3 octahedra, edges with two equivalent CrTe4Se2 octahedra, and faces with two equivalent CrTe3Se3 octahedra. The corner-sharing octahedra tilt angles range from 50–53°. All Cr–Te bond lengths are 2.79 Å. Both Cr–Se bond lengths are 2.59 Å. In the second Cr+2.67+ site, Cr+2.67+ is bonded to three equivalent Te2- and three equivalent Se2- atoms to form CrTe3Se3 octahedra that share corners with six equivalent CrTe4Se2 octahedra, edges with six equivalent CrTe3Se3 octahedra, and a faceface with one CrTe4Se2 octahedra. The corner-sharing octahedra tilt angles range from 50–53°. There are one shorter (2.82 Å) and two longer (2.84 Å) Cr–Te bond lengths. All Cr–Se bond lengths are 2.54 Å. Te2- is bonded in a 5-coordinate geometry to five Cr+2.67+ atoms. Se2- is bonded to four Cr+2.67+ atoms to form a mixture of corner and edge-sharing SeCr4 trigonal pyramids.

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Materials Data on Cr3(CuO6)2 by Materials Project

Cr3(CuO6)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Cr6+ sites. In the first Cr6+ site, Cr6+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with four CuO6 octahedra. The corner-sharing octahedra tilt angles range from 23–45°. There are a spread of Cr–O bond distances ranging from 1.66–1.68 Å. In the second Cr6+ site, Cr6+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with four CuO6 octahedra. The corner-sharing octahedra tilt angles range from 21–45°. There are a spread of Cr–O bond distances ranging from 1.66–1.68 Å. In the third Cr6+ site, Cr6+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with four CuO6 octahedra. The corner-sharing octahedra tilt angles range from 38–46°. There are a spread of Cr–O bond distances ranging from 1.66–1.68 Å. There are two inequivalent Cu3+ sites. In the first Cu3+ site, Cu3+ is bonded to six O2- atoms to form CuO6 octahedra that share corners with six CrO4 tetrahedra. There are a spread of Cu–O bond distances ranging from 1.96–2.05 Å. In the second Cu3+ site, Cu3+ is bonded to six O2- atoms to form CuO6 octahedra that share corners with six CrO4 tetrahedra. There are a spread of Cu–O bond distances ranging from 1.95–2.00 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the second O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the third O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Cr6+ and one Cu3+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the seventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the eighth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the ninth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the tenth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the eleventh O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom. In the twelfth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Cu3+ atom.

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Materials Data on Cr3(FeO6)2 by Materials Project

Cr3(FeO6)2 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are three inequivalent Cr6+ sites. In the first Cr6+ site, Cr6+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with four FeO6 octahedra. The corner-sharing octahedra tilt angles range from 20–41°. There is one shorter (1.66 Å) and three longer (1.67 Å) Cr–O bond length. In the second Cr6+ site, Cr6+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with four FeO6 octahedra. The corner-sharing octahedra tilt angles range from 19–42°. There are a spread of Cr–O bond distances ranging from 1.66–1.68 Å. In the third Cr6+ site, Cr6+ is bonded to four O2- atoms to form CrO4 tetrahedra that share corners with four FeO6 octahedra. The corner-sharing octahedra tilt angles range from 33–43°. There is one shorter (1.66 Å) and three longer (1.67 Å) Cr–O bond length. There are two inequivalent Fe3+ sites. In the first Fe3+ site, Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six CrO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.99–2.06 Å. In the second Fe3+ site, Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with six CrO4 tetrahedra. There are a spread of Fe–O bond distances ranging from 1.98–2.02 Å. There are twelve inequivalent O2- sites. In the first O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the second O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the third O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the fourth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the fifth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the sixth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the seventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the eighth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the ninth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the tenth O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the eleventh O2- site, O2- is bonded in a bent 150 degrees geometry to one Cr6+ and one Fe3+ atom. In the twelfth O2- site, O2- is bonded in a distorted bent 150 degrees geometry to one Cr6+ and one Fe3+ atom.

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Materials Data on Cr3(CoO6)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 Cr3(CoO6)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 Cr3(OF)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 Cr3(FeO4)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 Cr3(PO4)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 Cr3(FeO6)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 Cr3(P2O7)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 Cr3(P2O7)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 Cr3(OF)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 Cr3(P2O7)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 Cr3(CuO6)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 Cr3(NO5)2 by Materials Project

Cr3O10N2 crystallizes in the monoclinic P2_1/m space group. The structure is zero-dimensional and consists of twelve ammonia molecules and six Cr3O10 clusters. In each Cr3O10 cluster, there are two inequivalent Cr6+ sites. In the first Cr6+ site, Cr6+ is bonded to four O2- atoms to form corner-sharing CrO4 tetrahedra. There are a spread of Cr–O bond distances ranging from 1.63–1.78 Å. In the second Cr6+ site, Cr6+ is bonded to four O2- atoms to form corner-sharing CrO4 tetrahedra. There is two shorter (1.59 Å) and two longer (1.77 Å) Cr–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted bent 150 degrees geometry to two Cr6+ atoms. In the second O2- site, O2- is bonded in a single-bond geometry to one Cr6+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one Cr6+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one Cr6+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one Cr6+ atom. In the sixth O2- site, O2- is bonded in a single-bond geometry to one Cr6+ atom.

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