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At least 829 records · Page 46

Materials Data on PmDyRu2 by Materials Project

DyPmRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Dy is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Dy–Ru bond lengths are 2.99 Å. Pm is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Pm–Ru bond lengths are 2.99 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Dy and four equivalent Pm atoms.

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Materials Data on MgSbRu2 by Materials Project

MgRu2Sb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Mg is bonded in a body-centered cubic geometry to eight equivalent Ru and six equivalent Sb atoms. All Mg–Ru bond lengths are 2.73 Å. All Mg–Sb bond lengths are 3.15 Å. Ru is bonded in a distorted body-centered cubic geometry to four equivalent Mg and four equivalent Sb atoms. All Ru–Sb bond lengths are 2.73 Å. Sb is bonded in a 8-coordinate geometry to six equivalent Mg and eight equivalent Ru atoms.

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Materials Data on HoHfRu2 by Materials Project

HoHfRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ho is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ho–Ru bond lengths are 2.87 Å. Hf is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Hf–Ru bond lengths are 2.87 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Ho and four equivalent Hf atoms.

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Materials Data on Tb5(RuO6)2 by Materials Project

Tb5(RuO6)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Tb3+ sites. In the first Tb3+ site, Tb3+ is bonded to seven O2- atoms to form distorted TbO7 pentagonal bipyramids that share corners with two equivalent TbO6 octahedra, corners with two equivalent RuO6 octahedra, a cornercorner with one TbO7 pentagonal bipyramid, edges with two equivalent RuO6 octahedra, and edges with six TbO7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 43–56°. There are a spread of Tb–O bond distances ranging from 2.29–2.39 Å. In the second Tb3+ site, Tb3+ is bonded to seven O2- atoms to form distorted TbO7 pentagonal bipyramids that share corners with two equivalent TbO6 octahedra, a cornercorner with one TbO7 pentagonal bipyramid, an edgeedge with one TbO6 octahedra, edges with two equivalent RuO6 octahedra, and edges with six TbO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 54°. There are a spread of Tb–O bond distances ranging from 2.29–2.45 Å. In the third Tb3+ site, Tb3+ is bonded to six O2- atoms to form TbO6 octahedra that share corners with four equivalent RuO6 octahedra, corners with eight TbO7 pentagonal bipyramids, and edges with two equivalent TbO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 51°. There are four shorter (2.33 Å) and two longer (2.41 Å) Tb–O bond lengths. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with two equivalent TbO6 octahedra, corners with two equivalent TbO7 pentagonal bipyramids, edges with two equivalent RuO6 octahedra, and edges with four TbO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 51°. There are four shorter (2.00 Å) and two longer (2.02 Å) Ru–O bond lengths. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded to four Tb3+ atoms to form OTb4 tetrahedra that share corners with ten OTb4 tetrahedra, corners with three equivalent OTb2Ru2 trigonal pyramids, and edges with four OTb4 tetrahedra. In the second O2- site, O2- is bonded to three Tb3+ and one Ru+4.50+ atom to form distorted OTb3Ru tetrahedra that share corners with ten OTb4 tetrahedra, a cornercorner with one OTb2Ru2 trigonal pyramid, edges with three OTb4 tetrahedra, and edges with two equivalent OTb2Ru2 trigonal pyramids. In the third O2- site, O2- is bonded in a distorted trigonal planar geometry to one Tb3+ and two equivalent Ru+4.50+ atoms. In the fourth O2- site, O2- is bonded to two Tb3+ and two equivalent Ru+4.50+ atoms to form distorted OTb2Ru2 trigonal pyramids that share corners with eight OTb4 tetrahedra, edges with four equivalent OTb3Ru tetrahedra, and an edgeedge with one OTb2Ru2 trigonal pyramid.

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Materials Data on NdB2Ru3 by Materials Project

NdRu3B2 crystallizes in the hexagonal P6/mmm space group. The structure is three-dimensional. Nd is bonded in a 12-coordinate geometry to two equivalent Nd, twelve equivalent Ru, and six equivalent B atoms. Both Nd–Nd bond lengths are 3.05 Å. All Nd–Ru bond lengths are 3.18 Å. All Nd–B bond lengths are 3.22 Å. Ru is bonded in a distorted square co-planar geometry to four equivalent Nd and four equivalent B atoms. All Ru–B bond lengths are 2.22 Å. B is bonded in a 6-coordinate geometry to three equivalent Nd and six equivalent Ru atoms.

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Materials Data on ScRu3C by Materials Project

ScRu3C is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Sc is bonded to twelve equivalent Ru atoms to form ScRu12 cuboctahedra that share corners with twelve equivalent ScRu12 cuboctahedra, faces with six equivalent ScRu12 cuboctahedra, and faces with eight equivalent CRu6 octahedra. All Sc–Ru bond lengths are 2.89 Å. Ru is bonded in a distorted linear geometry to four equivalent Sc and two equivalent C atoms. Both Ru–C bond lengths are 2.04 Å. C is bonded to six equivalent Ru atoms to form CRu6 octahedra that share corners with six equivalent CRu6 octahedra and faces with eight equivalent ScRu12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.

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Materials Data on H2Ru6(CO)17 by Materials Project

(Ru)2(Ru2H)2(CO)17 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of thirty-four formaldehyde molecules, four ruthenium molecules, and two Ru2H clusters. In each Ru2H cluster, there are four inequivalent Ru2+ sites. In the first Ru2+ site, Ru2+ is bonded in a distorted single-bond geometry to one H1+ atom. The Ru–H bond length is 1.87 Å. In the second Ru2+ site, Ru2+ is bonded in a distorted single-bond geometry to one H1+ atom. The Ru–H bond length is 1.85 Å. In the third Ru2+ site, Ru2+ is bonded in a 2-coordinate geometry to two H1+ atoms. Both Ru–H bond lengths are 1.97 Å. In the fourth Ru2+ site, Ru2+ is bonded in a distorted L-shaped geometry to two H1+ atoms. There is one shorter (1.92 Å) and one longer (1.95 Å) Ru–H bond length. There are two inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a trigonal non-coplanar geometry to three Ru2+ atoms. In the second H1+ site, H1+ is bonded in a trigonal non-coplanar geometry to three Ru2+ atoms.

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Materials Data on Er6Te2Ru by Materials Project

Er6RuTe2 crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. there are two inequivalent Er sites. In the first Er site, Er is bonded in a 5-coordinate geometry to one Ru and four equivalent Te atoms. The Er–Ru bond length is 3.24 Å. All Er–Te bond lengths are 3.24 Å. In the second Er site, Er is bonded in a 4-coordinate geometry to two equivalent Ru and two equivalent Te atoms. Both Er–Ru bond lengths are 2.81 Å. Both Er–Te bond lengths are 3.22 Å. Ru is bonded in a 9-coordinate geometry to nine Er atoms. Te is bonded in a 9-coordinate geometry to nine Er atoms.

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Materials Data on LuSiRu by Materials Project

LuRuSi crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Lu is bonded in a 9-coordinate geometry to four equivalent Ru and five equivalent Si atoms. There are a spread of Lu–Ru bond distances ranging from 2.91–2.93 Å. There are a spread of Lu–Si bond distances ranging from 2.96–2.98 Å. Ru is bonded in a 8-coordinate geometry to four equivalent Lu and four equivalent Si atoms. There are a spread of Ru–Si bond distances ranging from 2.46–2.53 Å. Si is bonded in a 9-coordinate geometry to five equivalent Lu and four equivalent Ru atoms.

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Materials Data on LiRu2W by Materials Project

LiWRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a distorted body-centered cubic geometry to six equivalent W and eight equivalent Ru atoms. All Li–W bond lengths are 3.03 Å. All Li–Ru bond lengths are 2.62 Å. W is bonded in a 8-coordinate geometry to six equivalent Li and eight equivalent Ru atoms. All W–Ru bond lengths are 2.62 Å. Ru is bonded in a distorted body-centered cubic geometry to four equivalent Li and four equivalent W atoms.

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Materials Data on TaTiRu2 by Materials Project

TiTaRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ti is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ti–Ru bond lengths are 2.71 Å. Ta is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ta–Ru bond lengths are 2.71 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Ti and four equivalent Ta atoms.

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Materials Data on LiTaRu2 by Materials Project

LiTaRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Li is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Li–Ru bond lengths are 2.65 Å. Ta is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ta–Ru bond lengths are 2.65 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Li and four equivalent Ta atoms.

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Materials Data on TaAlRu2 by Materials Project

Ru2AlTa is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ta is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Ta–Ru bond lengths are 2.68 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Ta and four equivalent Al atoms. All Ru–Al bond lengths are 2.68 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ru atoms.

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Materials Data on ScSbRu2 by Materials Project

ScRu2Sb is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Sc is bonded in a body-centered cubic geometry to eight equivalent Ru and six equivalent Sb atoms. All Sc–Ru bond lengths are 2.77 Å. All Sc–Sb bond lengths are 3.20 Å. Ru is bonded in a distorted body-centered cubic geometry to four equivalent Sc and four equivalent Sb atoms. All Ru–Sb bond lengths are 2.77 Å. Sb is bonded in a distorted body-centered cubic geometry to six equivalent Sc and eight equivalent Ru atoms.

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Materials Data on BeRu2W by Materials Project

BeWRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a distorted body-centered cubic geometry to six equivalent W and eight equivalent Ru atoms. All Be–W bond lengths are 3.00 Å. All Be–Ru bond lengths are 2.59 Å. W is bonded in a 8-coordinate geometry to six equivalent Be and eight equivalent Ru atoms. All W–Ru bond lengths are 2.59 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Be and four equivalent W atoms.

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Materials Data on BeGeRu2 by Materials Project

BeRu2Ge is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Be is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Be–Ru bond lengths are 2.53 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Be and four equivalent Ge atoms. All Ru–Ge bond lengths are 2.53 Å. Ge is bonded in a body-centered cubic geometry to eight equivalent Ru atoms.

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Materials Data on TmPaRu2 by Materials Project

PaTmRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Pa is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Pa–Ru bond lengths are 2.95 Å. Tm is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Tm–Ru bond lengths are 2.95 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Pa and four equivalent Tm atoms.

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Materials Data on AlSiRu2 by Materials Project

Ru2AlSi is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Ru is bonded in a body-centered cubic geometry to four equivalent Al and four equivalent Si atoms. All Ru–Al bond lengths are 2.57 Å. All Ru–Si bond lengths are 2.57 Å. Al is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. Si is bonded in a body-centered cubic geometry to eight equivalent Ru atoms.

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