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At least 1,513 records · Page 84

Materials Data on Tl3Ru by Materials Project

RuTl3 is beta Cu3Ti-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ru is bonded to twelve equivalent Tl atoms to form RuTl12 cuboctahedra that share corners with six equivalent RuTl12 cuboctahedra, corners with twelve equivalent TlTl8Ru4 cuboctahedra, edges with eighteen equivalent TlTl8Ru4 cuboctahedra, faces with eight equivalent RuTl12 cuboctahedra, and faces with twelve equivalent TlTl8Ru4 cuboctahedra. All Ru–Tl bond lengths are 3.19 Å. Tl is bonded to four equivalent Ru and eight equivalent Tl atoms to form distorted TlTl8Ru4 cuboctahedra that share corners with four equivalent RuTl12 cuboctahedra, corners with fourteen equivalent TlTl8Ru4 cuboctahedra, edges with six equivalent RuTl12 cuboctahedra, edges with twelve equivalent TlTl8Ru4 cuboctahedra, faces with four equivalent RuTl12 cuboctahedra, and faces with sixteen equivalent TlTl8Ru4 cuboctahedra. There are a spread of Tl–Tl bond distances ranging from 3.08–3.30 Å.

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Materials Data on V2ReRu by Materials Project

V2ReRu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. V is bonded in a body-centered cubic geometry to four equivalent Re and four equivalent Ru atoms. All V–Re bond lengths are 2.62 Å. All V–Ru bond lengths are 2.62 Å. Re is bonded in a distorted body-centered cubic geometry to eight equivalent V atoms. Ru is bonded in a body-centered cubic geometry to eight equivalent V atoms.

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Materials Data on Nb2RuW by Materials Project

Nb2WRu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Nb is bonded in a body-centered cubic geometry to four equivalent W and four equivalent Ru atoms. All Nb–W bond lengths are 2.79 Å. All Nb–Ru bond lengths are 2.79 Å. W is bonded in a body-centered cubic geometry to eight equivalent Nb atoms. Ru is bonded in a body-centered cubic geometry to eight equivalent Nb atoms.

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Materials Data on Ba(Sb3Ru)4 by Materials Project

BaRu4Sb12 crystallizes in the cubic Im-3 space group. The structure is three-dimensional. Ba2+ is bonded to twelve equivalent Sb1- atoms to form BaSb12 cuboctahedra that share faces with eight equivalent RuSb6 octahedra. All Ba–Sb bond lengths are 3.58 Å. Ru+2.50+ is bonded to six equivalent Sb1- atoms to form RuSb6 octahedra that share corners with six equivalent RuSb6 octahedra and faces with two equivalent BaSb12 cuboctahedra. The corner-sharing octahedral tilt angles are 55°. All Ru–Sb bond lengths are 2.66 Å. Sb1- is bonded in a 2-coordinate geometry to one Ba2+, two equivalent Ru+2.50+, and two equivalent Sb1- atoms. There are one shorter (2.95 Å) and one longer (3.03 Å) Sb–Sb bond lengths.

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Materials Data on HfRu3 by Materials Project

HfRu3 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Hf is bonded to twelve equivalent Ru atoms to form a mixture of corner and face-sharing HfRu12 cuboctahedra. All Hf–Ru bond lengths are 2.80 Å. Ru is bonded in a distorted square co-planar geometry to four equivalent Hf atoms.

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Materials Data on Al2Ru by Materials Project

RuAl2 crystallizes in the tetragonal I4/mmm space group. The structure is three-dimensional. Ru is bonded in a 8-coordinate geometry to ten equivalent Al atoms. There are eight shorter (2.61 Å) and two longer (2.88 Å) Ru–Al bond lengths. Al is bonded in a 10-coordinate geometry to five equivalent Ru atoms.

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Materials Data on ZrRu3 by Materials Project

ZrRu3 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Zr is bonded to twelve equivalent Ru atoms to form a mixture of corner and face-sharing ZrRu12 cuboctahedra. All Zr–Ru bond lengths are 2.81 Å. Ru is bonded in a distorted square co-planar geometry to four equivalent Zr atoms.

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Materials Data on Er2Mg3Ru by Materials Project

Mg3Er2Ru crystallizes in the tetragonal P4/mmm space group. The structure is three-dimensional. there are two inequivalent Mg sites. In the first Mg site, Mg is bonded to eight Mg and four equivalent Er atoms to form a mixture of edge, corner, and face-sharing MgEr4Mg8 cuboctahedra. There are four shorter (3.14 Å) and four longer (3.36 Å) Mg–Mg bond lengths. All Mg–Er bond lengths are 3.48 Å. In the second Mg site, Mg is bonded to twelve Mg atoms to form MgMg12 cuboctahedra that share corners with four equivalent MgMg12 cuboctahedra, edges with sixteen equivalent MgEr4Mg8 cuboctahedra, and faces with sixteen MgEr4Mg8 cuboctahedra. All Mg–Mg bond lengths are 3.36 Å. Er is bonded in a 4-coordinate geometry to four equivalent Mg and four equivalent Ru atoms. All Er–Ru bond lengths are 2.89 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Er atoms.

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Materials Data on Ce(As3Ru)4 by Materials Project

CeRu4As12 crystallizes in the cubic Im-3 space group. The structure is three-dimensional. Ce3+ is bonded to twelve equivalent As+1.67- atoms to form CeAs12 cuboctahedra that share faces with eight equivalent RuAs6 octahedra. All Ce–As bond lengths are 3.25 Å. Ru+4.25+ is bonded to six equivalent As+1.67- atoms to form RuAs6 octahedra that share corners with six equivalent RuAs6 octahedra and faces with two equivalent CeAs12 cuboctahedra. The corner-sharing octahedral tilt angles are 58°. All Ru–As bond lengths are 2.46 Å. As+1.67- is bonded in a 5-coordinate geometry to one Ce3+, two equivalent Ru+4.25+, and two equivalent As+1.67- atoms. There are one shorter (2.58 Å) and one longer (2.63 Å) As–As bond lengths.

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Materials Data on GeRu by Materials Project

RuGe crystallizes in the cubic P2_13 space group. The structure is three-dimensional. Ru is bonded in a 4-coordinate geometry to seven equivalent Ge atoms. There are a spread of Ru–Ge bond distances ranging from 2.47–2.82 Å. Ge is bonded in a 7-coordinate geometry to seven equivalent Ru atoms.

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Materials Data on Sr4Li(RuO4)3 by Materials Project

LiSr4(RuO4)3 is Orthorhombic Perovskite-derived structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with six RuO6 octahedra. The corner-sharing octahedra tilt angles range from 11–17°. There are four shorter (2.04 Å) and two longer (2.12 Å) Li–O bond lengths. There are two inequivalent Sr2+ sites. In the first Sr2+ site, Sr2+ is bonded in a 12-coordinate geometry to ten O2- atoms. There are a spread of Sr–O bond distances ranging from 2.51–2.95 Å. In the second Sr2+ site, Sr2+ is bonded in a 11-coordinate geometry to eleven O2- atoms. There are a spread of Sr–O bond distances ranging from 2.49–3.13 Å. There are three inequivalent Ru5+ sites. In the first Ru5+ site, Ru5+ is bonded to six O2- atoms to form corner-sharing RuO6 octahedra. The corner-sharing octahedra tilt angles range from 19–21°. There are a spread of Ru–O bond distances ranging from 1.99–2.03 Å. In the second Ru5+ site, Ru5+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with two equivalent LiO6 octahedra and corners with four equivalent RuO6 octahedra. The corner-sharing octahedra tilt angles range from 17–21°. There are a spread of Ru–O bond distances ranging from 1.91–2.02 Å. In the third Ru5+ site, Ru5+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with two equivalent RuO6 octahedra and corners with four equivalent LiO6 octahedra. The corner-sharing octahedra tilt angles range from 11–20°. There is four shorter (1.93 Å) and two longer (2.03 Å) Ru–O bond length. There are six inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to one Li1+, four Sr2+, and one Ru5+ atom. In the second O2- site, O2- is bonded in a 5-coordinate geometry to three Sr2+ and two Ru5+ atoms. In the third O2- site, O2- is bonded in a 5-coordinate geometry to three Sr2+ and two Ru5+ atoms. In the fourth O2- site, O2- is bonded in a 6-coordinate geometry to one Li1+, four Sr2+, and one Ru5+ atom. In the fifth O2- site, O2- is bonded in a 5-coordinate geometry to one Li1+, three Sr2+, and one Ru5+ atom. In the sixth O2- site, O2- is bonded in a 5-coordinate geometry to four Sr2+ and two Ru5+ atoms.

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Materials Data on TmRu3 by Materials Project

TmRu3 is Uranium Silicide structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Tm is bonded to twelve equivalent Ru atoms to form a mixture of corner and face-sharing TmRu12 cuboctahedra. All Tm–Ru bond lengths are 2.84 Å. Ru is bonded in a distorted square co-planar geometry to four equivalent Tm atoms.

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Materials Data on Ho(BRu)4 by Materials Project

Ho(RuB)4 crystallizes in the tetragonal I4_1/acd space group. The structure is three-dimensional. Ho3+ is bonded in a 12-coordinate geometry to twelve equivalent B3- atoms. There are a spread of Ho–B bond distances ranging from 2.95–3.22 Å. Ru+2.25+ is bonded to five equivalent B3- atoms to form a mixture of distorted corner and edge-sharing RuB5 trigonal bipyramids. There are a spread of Ru–B bond distances ranging from 2.15–2.29 Å. B3- is bonded in a 6-coordinate geometry to three equivalent Ho3+, five equivalent Ru+2.25+, and one B3- atom. The B–B bond length is 1.79 Å.

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Materials Data on Gd2IrRu by Materials Project

Gd2RuIr is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Gd is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Ir atoms. All Gd–Ru bond lengths are 2.98 Å. All Gd–Ir bond lengths are 2.98 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Gd atoms. Ir is bonded in a body-centered cubic geometry to eight equivalent Gd atoms.

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Materials Data on La2RuAu by Materials Project

La2RuAu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. La is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Au atoms. All La–Ru bond lengths are 3.18 Å. All La–Au bond lengths are 3.18 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent La atoms. Au is bonded in a body-centered cubic geometry to eight equivalent La atoms.

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Materials Data on Ta2MnRu by Materials Project

Ta2MnRu crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Ta2MnRu ribbons oriented in the (1, 0, 0) direction. Ta is bonded in a linear geometry to one Mn and one Ru atom. The Ta–Mn bond length is 2.19 Å. The Ta–Ru bond length is 2.24 Å. Mn is bonded in a linear geometry to two equivalent Ta atoms. Ru is bonded in a linear geometry to two equivalent Ta atoms.

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Materials Data on Al2OsRu by Materials Project

OsRuAl2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two OsRuAl2 ribbons oriented in the (1, 0, 0) direction. Os is bonded in a linear geometry to two equivalent Al atoms. Both Os–Al bond lengths are 2.43 Å. Ru is bonded in a linear geometry to two equivalent Al atoms. Both Ru–Al bond lengths are 2.43 Å. Al is bonded in a linear geometry to one Os and one Ru atom.

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Materials Data on Tb2PdRu by Materials Project

Tb2RuPd is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Tb is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Pd atoms. All Tb–Ru bond lengths are 3.00 Å. All Tb–Pd bond lengths are 3.00 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Tb atoms. Pd is bonded in a body-centered cubic geometry to eight equivalent Tb atoms.

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