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At least 1,153 records · Page 64
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DOE OSTI2020

Materials Data on NpScRu2 by Materials Project

NpScRu2 is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Np is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Np–Ru bond lengths are 2.84 Å. Sc is bonded in a body-centered cubic geometry to eight equivalent Ru atoms. All Sc–Ru bond lengths are 2.84 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Np and four equivalent Sc atoms.

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Materials Data on VTeRu by Materials Project

VRuTe is half-Heusler structured and crystallizes in the cubic F-43m space group. The structure is three-dimensional. V is bonded to four equivalent Ru and six equivalent Te atoms to form a mixture of distorted face and corner-sharing VTe6Ru4 tetrahedra. All V–Ru bond lengths are 2.63 Å. All V–Te bond lengths are 3.04 Å. Ru is bonded in a body-centered cubic geometry to four equivalent V and four equivalent Te atoms. All Ru–Te bond lengths are 2.63 Å. Te is bonded in a 10-coordinate geometry to six equivalent V and four equivalent Ru atoms.

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Materials Data on ZrSnRu2 by Materials Project

ZrRu2Sn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Zr is bonded in a body-centered cubic geometry to eight equivalent Ru and six equivalent Sn atoms. All Zr–Ru bond lengths are 2.81 Å. All Zr–Sn bond lengths are 3.24 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Zr and four equivalent Sn atoms. All Ru–Sn bond lengths are 2.81 Å. Sn is bonded in a distorted body-centered cubic geometry to six equivalent Zr and eight equivalent Ru atoms.

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Materials Data on Be2Ru by Materials Project

Be2Ru is Hexagonal Laves structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Be sites. In the first Be site, Be is bonded to six equivalent Be and six equivalent Ru atoms to form a mixture of face, edge, and corner-sharing BeBe6Ru6 cuboctahedra. All Be–Be bond lengths are 2.18 Å. All Be–Ru bond lengths are 2.55 Å. In the second Be site, Be is bonded to six Be and six equivalent Ru atoms to form a mixture of face, edge, and corner-sharing BeBe6Ru6 cuboctahedra. There are two shorter (2.15 Å) and two longer (2.21 Å) Be–Be bond lengths. There are two shorter (2.51 Å) and four longer (2.56 Å) Be–Ru bond lengths. Ru is bonded in a 12-coordinate geometry to twelve Be atoms.

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Materials Data on LiNbRu2 by Materials Project

LiNbRu2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two LiNbRu2 ribbons oriented in the (1, 0, 0) direction. Li is bonded in a linear geometry to two equivalent Ru atoms. Both Li–Ru bond lengths are 2.71 Å. Nb is bonded in a linear geometry to two equivalent Ru atoms. Both Nb–Ru bond lengths are 2.18 Å. Ru is bonded in a linear geometry to one Li and one Nb atom.

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Materials Data on Pr3Ge13Ru4 by Materials Project

Pr3Ru4Ge13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Pr is bonded in a 12-coordinate geometry to four equivalent Ru and twelve equivalent Ge atoms. All Pr–Ru bond lengths are 3.24 Å. There are eight shorter (3.25 Å) and four longer (3.27 Å) Pr–Ge bond lengths. Ru is bonded in a 6-coordinate geometry to three equivalent Pr and six equivalent Ge atoms. All Ru–Ge bond lengths are 2.51 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 2-coordinate geometry to three equivalent Pr, two equivalent Ru, and one Ge atom. The Ge–Ge bond length is 3.03 Å. In the second Ge site, Ge is bonded in a cuboctahedral geometry to twelve equivalent Ge atoms.

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DOE OSTI2020

Materials Data on ZrSbRu2 by Materials Project

Ru2ZrSb crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Ru2ZrSb ribbons oriented in the (1, 0, 0) direction. Zr is bonded in a linear geometry to two equivalent Ru atoms. Both Zr–Ru bond lengths are 2.24 Å. Ru is bonded in a linear geometry to one Zr and one Sb atom. The Ru–Sb bond length is 2.51 Å. Sb is bonded in a linear geometry to two equivalent Ru atoms.

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DOE OSTI2020

Materials Data on MnBe2Ru by Materials Project

Be2MnRu 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 four equivalent Mn and four equivalent Ru atoms. All Be–Mn bond lengths are 2.40 Å. All Be–Ru bond lengths are 2.40 Å. Mn is bonded in a 8-coordinate geometry to eight equivalent Be and six equivalent Ru atoms. All Mn–Ru bond lengths are 2.77 Å. Ru is bonded in a distorted body-centered cubic geometry to eight equivalent Be and six equivalent Mn atoms.

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Materials Data on ZrTaRu2 by Materials Project

ZrTaRu2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two ZrTaRu2 ribbons oriented in the (1, 0, 0) direction. Zr is bonded in a linear geometry to two equivalent Ru atoms. Both Zr–Ru bond lengths are 2.31 Å. Ta is bonded in a linear geometry to two equivalent Ru atoms. Both Ta–Ru bond lengths are 2.21 Å. Ru is bonded in a linear geometry to one Zr and one Ta atom.

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Materials Data on NbSnRu2 by Materials Project

NbRu2Sn 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 eight equivalent Ru atoms. All Nb–Ru bond lengths are 2.77 Å. Ru is bonded in a body-centered cubic geometry to four equivalent Nb and four equivalent Sn atoms. All Ru–Sn bond lengths are 2.77 Å. Sn is bonded in a distorted body-centered cubic geometry to eight equivalent Ru atoms.

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Materials Data on HfZrRu2 by Materials Project

HfZrRu2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two HfZrRu2 ribbons oriented in the (1, 0, 0) direction. Hf is bonded in a linear geometry to two equivalent Ru atoms. Both Hf–Ru bond lengths are 2.30 Å. Zr is bonded in a linear geometry to two equivalent Ru atoms. Both Zr–Ru bond lengths are 2.28 Å. Ru is bonded in a linear geometry to one Hf and one Zr atom.

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DOE OSTI2020

Materials Data on Yb3Ge13Ru4 by Materials Project

Yb3Ru4Ge13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. Yb is bonded in a 8-coordinate geometry to four equivalent Ru and twelve equivalent Ge atoms. All Yb–Ru bond lengths are 3.19 Å. There are eight shorter (3.13 Å) and four longer (3.22 Å) Yb–Ge bond lengths. Ru is bonded in a 9-coordinate geometry to three equivalent Yb and six equivalent Ge atoms. All Ru–Ge bond lengths are 2.50 Å. There are two inequivalent Ge sites. In the first Ge site, Ge is bonded in a 6-coordinate geometry to three equivalent Yb, two equivalent Ru, and two Ge atoms. There are one shorter (2.68 Å) and one longer (3.11 Å) Ge–Ge bond lengths. In the second Ge site, Ge is bonded in a cuboctahedral geometry to twelve equivalent Ge atoms.

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Materials Data on TiVRu2 by Materials Project

TiVRu2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two TiVRu2 ribbons oriented in the (1, 0, 0) direction. Ti is bonded in a linear geometry to two equivalent Ru atoms. Both Ti–Ru bond lengths are 2.17 Å. V is bonded in a linear geometry to two equivalent Ru atoms. Both V–Ru bond lengths are 2.12 Å. Ru is bonded in a linear geometry to one Ti and one V atom.

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Materials Data on AlRu2W by Materials Project

WRu2Al crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two WRu2Al ribbons oriented in the (1, 0, 0) direction. W is bonded in a linear geometry to two equivalent Ru atoms. Both W–Ru bond lengths are 2.13 Å. Ru is bonded in a linear geometry to one W and one Al atom. The Ru–Al bond length is 2.51 Å. Al is bonded in a linear geometry to two equivalent Ru atoms.

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Materials Data on La3Sn13Ru4 by Materials Project

La3Ru4Sn13 crystallizes in the cubic Pm-3n space group. The structure is three-dimensional. La is bonded in a 12-coordinate geometry to four equivalent Ru and twelve equivalent Sn atoms. All La–Ru bond lengths are 3.49 Å. There are four shorter (3.45 Å) and eight longer (3.50 Å) La–Sn bond lengths. Ru is bonded in a 6-coordinate geometry to three equivalent La and six equivalent Sn atoms. All Ru–Sn bond lengths are 2.69 Å. There are two inequivalent Sn sites. In the first Sn site, Sn is bonded in a 2-coordinate geometry to three equivalent La, two equivalent Ru, and one Sn atom. The Sn–Sn bond length is 3.35 Å. In the second Sn site, Sn is bonded in a cuboctahedral geometry to twelve equivalent Sn atoms.

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Materials Data on TaGeRu2 by Materials Project

TaRu2Ge crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two TaRu2Ge ribbons oriented in the (1, 0, 0) direction. Ta is bonded in a linear geometry to two equivalent Ru atoms. Both Ta–Ru bond lengths are 2.18 Å. Ru is bonded in a linear geometry to one Ta and one Ge atom. The Ru–Ge bond length is 2.37 Å. Ge is bonded in a linear geometry to two equivalent Ru atoms.

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DOE OSTI2020

Materials Data on AlSnRu2 by Materials Project

Ru2AlSn crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Ru2AlSn ribbons oriented in the (1, 0, 0) direction. Ru is bonded in a linear geometry to one Al and one Sn atom. The Ru–Al bond length is 2.43 Å. The Ru–Sn bond length is 2.56 Å. Al is bonded in a linear geometry to two equivalent Ru atoms. Sn is bonded in a linear geometry to two equivalent Ru atoms.

36 MATERIALS SCIENCE↗
DOE OSTI2020

Materials Data on Ga2NiRu by Materials Project

RuNiGa2 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 six equivalent Ni and eight equivalent Ga atoms. All Ru–Ni bond lengths are 2.98 Å. All Ru–Ga bond lengths are 2.58 Å. Ni is bonded in a distorted body-centered cubic geometry to six equivalent Ru and eight equivalent Ga atoms. All Ni–Ga bond lengths are 2.58 Å. Ga is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Ni atoms.

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