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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
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
IrCl6(IrN3Cl2)2(N2)2 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of four nitrogen molecules, two IrCl6 clusters, and four IrN3Cl2 clusters. In each IrCl6 cluster, Ir4+ is bonded in an octahedral geometry to six Cl1- atoms. There are a spread of Ir–Cl bond distances ranging from 2.29–2.33 Å. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom. In the third Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom. In each IrN3Cl2 cluster, Ir4+ is bonded in a tetrahedral geometry to three N+0.20- and one Cl1- atom. There is two shorter (1.73 Å) and one longer (2.01 Å) Ir–N bond length. The Ir–Cl bond length is 2.28 Å. There are two inequivalent N+0.20- sites. In the first N+0.20- site, N+0.20- is bonded in a bent 120 degrees geometry to one Ir4+ and one Cl1- atom. The N–Cl bond length is 1.66 Å. In the second N+0.20- site, N+0.20- is bonded in a single-bond geometry to one Ir4+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one N+0.20- atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom.
IrCl6(CoN3Cl)2(N2)2Cl2 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of two chlorine molecules, four nitrogen molecules, four CoN3Cl clusters, and two IrCl6 clusters. In each CoN3Cl cluster, Co2+ is bonded in a distorted trigonal non-coplanar geometry to three N+0.20+ atoms. There is one shorter (1.60 Å) and two longer (1.78 Å) Co–N bond length. There are two inequivalent N+0.20+ sites. In the first N+0.20+ site, N+0.20+ is bonded in a distorted water-like geometry to one Co2+ and one Cl1- atom. The N–Cl bond length is 1.74 Å. In the second N+0.20+ site, N+0.20+ is bonded in a single-bond geometry to one Co2+ atom. Cl1- is bonded in an L-shaped geometry to two equivalent N+0.20+ atoms. In each IrCl6 cluster, Ir4+ is bonded in an octahedral geometry to six Cl1- atoms. There are a spread of Ir–Cl bond distances ranging from 2.30–2.33 Å. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom. In the third Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom.
Sr3TiGa10O20 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 5-coordinate geometry to seven O2- atoms. There are a spread of Sr–O bond distances ranging from 2.48–3.09 Å. In the second Sr2+ site, Sr2+ is bonded in a 6-coordinate geometry to six O2- atoms. There are two shorter (2.51 Å) and four longer (2.75 Å) Sr–O bond lengths. Ti4+ is bonded to six O2- atoms to form TiO6 octahedra that share corners with four equivalent GaO4 tetrahedra and edges with four equivalent GaO6 octahedra. There is two shorter (1.94 Å) and four longer (2.01 Å) Ti–O bond length. There are three inequivalent Ga3+ sites. In the first Ga3+ site, Ga3+ is bonded to four O2- atoms to form GaO4 tetrahedra that share a cornercorner with one GaO6 octahedra and corners with four GaO4 tetrahedra. The corner-sharing octahedral tilt angles are 52°. There are a spread of Ga–O bond distances ranging from 1.84–1.88 Å. In the second Ga3+ site, Ga3+ is bonded to six O2- atoms to form GaO6 octahedra that share corners with six GaO4 tetrahedra, an edgeedge with one GaO6 octahedra, and edges with two equivalent TiO6 octahedra. There are a spread of Ga–O bond distances ranging from 1.96–2.09 Å. In the third Ga3+ site, Ga3+ is bonded to four O2- atoms to form GaO4 tetrahedra that share a cornercorner with one TiO6 octahedra, corners with two equivalent GaO6 octahedra, and corners with three equivalent GaO4 tetrahedra. The corner-sharing octahedra tilt angles range from 45–63°. There are a spread of Ga–O bond distances ranging from 1.84–1.89 Å. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three Ga3+ atoms. In the second O2- site, O2- is bonded in a distorted trigonal planar geometry to one Sr2+ and two Ga3+ atoms. In the third O2- site, O2- is bonded to one Sr2+, one Ti4+, and two equivalent Ga3+ atoms to form a mixture of distorted edge and corner-sharing OSrTiGa2 tetrahedra. In the fourth O2- site, O2- is bonded to two Sr2+ and two Ga3+ atoms to form distorted OSr2Ga2 tetrahedra that share corners with three OSrTiGa2 tetrahedra and an edgeedge with one OSr2Ga2 tetrahedra. In the fifth O2- site, O2- is bonded in a distorted trigonal planar geometry to one Sr2+ and two equivalent Ga3+ atoms. In the sixth O2- site, O2- is bonded in a 3-coordinate geometry to one Sr2+, one Ti4+, and two Ga3+ atoms.
ReCl6(RuN5H15Cl)2Cl2 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of two hexachlororhenium molecules, four hydrochloric acid molecules, and four RuN5H15Cl clusters. In each RuN5H15Cl cluster, Ru+3.50+ is bonded in an octahedral geometry to five N3- and one Cl1- atom. There are a spread of Ru–N bond distances ranging from 2.12–2.14 Å. The Ru–Cl bond length is 2.33 Å. There are three inequivalent N3- sites. In the first N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Ru+3.50+ and three H1+ atoms. All N–H bond lengths are 1.03 Å. In the second N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Ru+3.50+ and three H1+ atoms. All N–H bond lengths are 1.03 Å. In the third N3- site, N3- is bonded in a distorted trigonal non-coplanar geometry to one Ru+3.50+ and three H1+ atoms. There is two shorter (1.03 Å) and one longer (1.04 Å) N–H bond length. There are eight inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one N3- atom. Cl1- is bonded in a single-bond geometry to one Ru+3.50+ atom.
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
RhNPdN4(NO2)5 crystallizes in the monoclinic P2_1/m space group. The structure is zero-dimensional and consists of two azanide;palladium molecules, ten nitrous acid molecules, and two RhN clusters. In each RhN cluster, Rh4+ is bonded in a single-bond geometry to one N+1.40+ atom. The Rh–N bond length is 1.66 Å. N+1.40+ is bonded in a single-bond geometry to one Rh4+ atom.
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
PtCl6(IrN5Cl2)2 is Krennerite-like structured and crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of four IrN5Cl2 clusters and two PtCl6 clusters. In each IrN5Cl2 cluster, Ir5+ is bonded in a 6-coordinate geometry to five N+0.60- and one Cl1- atom. There are a spread of Ir–N bond distances ranging from 1.80–2.31 Å. The Ir–Cl bond length is 2.44 Å. There are three inequivalent N+0.60- sites. In the first N+0.60- site, N+0.60- is bonded in an L-shaped geometry to one Ir5+ and one Cl1- atom. The N–Cl bond length is 1.54 Å. In the second N+0.60- site, N+0.60- is bonded in a single-bond geometry to one Ir5+ atom. In the third N+0.60- site, N+0.60- is bonded in a single-bond geometry to one Ir5+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a bent 120 degrees geometry to two equivalent N+0.60- atoms. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir5+ atom. In each PtCl6 cluster, Pt6+ is bonded in an octahedral geometry to six Cl1- atoms. There are two shorter (2.33 Å) and four longer (2.34 Å) Pt–Cl bond lengths. There are three inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one Pt6+ atom. In the second Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Pt6+ atom. In the third Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Pt6+ atom.
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
ReMn(CO)5(CO)5 crystallizes in the monoclinic C2 space group. The structure is zero-dimensional and consists of twenty formaldehyde molecules, four rhenium molecules, and four Mn(CO)5 clusters. In each Mn(CO)5 cluster, Mn2+ is bonded in a square pyramidal geometry to five C+1.40+ atoms. There are a spread of Mn–C bond distances ranging from 1.81–1.87 Å. There are five inequivalent C+1.40+ sites. In the first C+1.40+ site, C+1.40+ is bonded in a linear geometry to one Mn2+ and one O2- atom. The C–O bond length is 1.16 Å. In the second C+1.40+ site, C+1.40+ is bonded in a linear geometry to one Mn2+ and one O2- atom. The C–O bond length is 1.16 Å. In the third C+1.40+ site, C+1.40+ is bonded in a linear geometry to one Mn2+ and one O2- atom. The C–O bond length is 1.16 Å. In the fourth C+1.40+ site, C+1.40+ is bonded in a linear geometry to one Mn2+ and one O2- atom. The C–O bond length is 1.16 Å. In the fifth C+1.40+ site, C+1.40+ is bonded in a linear geometry to one Mn2+ and one O2- atom. The C–O bond length is 1.16 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C+1.40+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C+1.40+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C+1.40+ atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C+1.40+ atom. In the fifth O2- site, O2- is bonded in a single-bond geometry to one C+1.40+ atom.
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
ReCl6(IrN5Cl2)2 is Calaverite-like structured and crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of two hexachlororhenium molecules and four IrN5Cl2 clusters. In each IrN5Cl2 cluster, Ir+4.50+ is bonded in a 3-coordinate geometry to five N+0.60- and one Cl1- atom. There are a spread of Ir–N bond distances ranging from 1.78–2.36 Å. The Ir–Cl bond length is 2.52 Å. There are three inequivalent N+0.60- sites. In the first N+0.60- site, N+0.60- is bonded in a single-bond geometry to one Ir+4.50+ atom. In the second N+0.60- site, N+0.60- is bonded in a distorted L-shaped geometry to one Ir+4.50+ and one Cl1- atom. The N–Cl bond length is 1.53 Å. In the third N+0.60- site, N+0.60- is bonded in a single-bond geometry to one Ir+4.50+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Ir+4.50+ atom. In the second Cl1- site, Cl1- is bonded in a bent 120 degrees geometry to two equivalent N+0.60- atoms.
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
OsCl6(IrN3Cl2)2(N2)2 crystallizes in the monoclinic C2/m space group. The structure is zero-dimensional and consists of two hexachloroosmium molecules, four nitrogen molecules, and four IrN3Cl2 clusters. In each IrN3Cl2 cluster, Ir4+ is bonded in a tetrahedral geometry to three N+0.60- and one Cl1- atom. There is two shorter (1.73 Å) and one longer (2.00 Å) Ir–N bond length. The Ir–Cl bond length is 2.27 Å. There are two inequivalent N+0.60- sites. In the first N+0.60- site, N+0.60- is bonded in a bent 120 degrees geometry to one Ir4+ and one Cl1- atom. The N–Cl bond length is 1.67 Å. In the second N+0.60- site, N+0.60- is bonded in a single-bond geometry to one Ir4+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a single-bond geometry to one N+0.60- atom. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ir4+ atom.
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
ReCl6(RuN3Cl2)2(N2)2 crystallizes in the monoclinic C2/m space group. The structure is one-dimensional and consists of two hexachlororhenium molecules; four nitrogen molecules; and two RuN3Cl2 ribbons oriented in the (0, 1, 0) direction. In each RuN3Cl2 ribbon, Ru+4.50+ is bonded in a trigonal non-coplanar geometry to three N+0.60- atoms. There is two shorter (1.71 Å) and one longer (1.82 Å) Ru–N bond length. There are two inequivalent N+0.60- sites. In the first N+0.60- site, N+0.60- is bonded in a single-bond geometry to one Ru+4.50+ and one Cl1- atom. The N–Cl bond length is 3.32 Å. In the second N+0.60- site, N+0.60- is bonded in a bent 150 degrees geometry to one Ru+4.50+ and one Cl1- atom. The N–Cl bond length is 1.60 Å. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 1-coordinate geometry to two equivalent N+0.60- and one Cl1- atom. The Cl–Cl bond length is 1.99 Å. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one N+0.60- atom.