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Materials Data on RuO4 by Materials Project

RuO4 is Silicon tetrafluoride-like structured and crystallizes in the monoclinic C2/c space group. The structure is zero-dimensional and consists of four ruthenium(iv) hydroxide molecules. Ru is bonded in a tetrahedral geometry to four O atoms. All Ru–O bond lengths are 1.71 Å. There are two inequivalent O sites. In the first O site, O is bonded in a single-bond geometry to one Ru atom. In the second O site, O is bonded in a single-bond geometry to one Ru atom.

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Materials Data on Ba3LuRu2O9 by Materials Project

Ba3LuRu2O9 is (Cubic) Perovskite-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with nine BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, faces with three equivalent LuO6 octahedra, and faces with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 14°. There are a spread of Ba–O bond distances ranging from 2.91–3.05 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent LuO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (2.96 Å) and six longer (2.97 Å) Ba–O bond lengths. Lu3+ is bonded to six equivalent O2- atoms to form LuO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 1°. All Lu–O bond lengths are 2.18 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent LuO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (1.98 Å) and three longer (2.04 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Lu3+, and one Ru+4.50+ atom. In the second O2- site, O2- is bonded in a 6-coordinate geometry to four Ba2+ and two equivalent Ru+4.50+ atoms.

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Materials Data on Ba3EuRu2O9 by Materials Project

Ba3EuRu2O9 is (Cubic) Perovskite-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with nine BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, faces with three equivalent EuO6 octahedra, and faces with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 14°. There are a spread of Ba–O bond distances ranging from 2.89–3.22 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent EuO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (2.99 Å) and six longer (3.01 Å) Ba–O bond lengths. Eu3+ is bonded to six equivalent O2- atoms to form EuO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 2°. All Eu–O bond lengths are 2.30 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent EuO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (1.94 Å) and three longer (2.06 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Eu3+, and one Ru+4.50+ atom. In the second O2- site, O2- is bonded in a 6-coordinate geometry to four Ba2+ and two equivalent Ru+4.50+ atoms.

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Materials Data on Ba3LaRu2O9 by Materials Project

Ba3LaRu2O9 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded in a 12-coordinate geometry to twelve O2- atoms. There are a spread of Ba–O bond distances ranging from 2.85–3.42 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with six equivalent BaO12 cuboctahedra, faces with two equivalent LaO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (3.00 Å) and six longer (3.01 Å) Ba–O bond lengths. La3+ is bonded to six equivalent O2- atoms to form LaO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with two equivalent BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 3°. All La–O bond lengths are 2.34 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent LaO6 octahedra, faces with three equivalent BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 3°. There are three shorter (1.95 Å) and three longer (2.06 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four Ba2+ and two equivalent Ru+4.50+ atoms to form a mixture of distorted face and corner-sharing OBa4Ru2 octahedra. The corner-sharing octahedra tilt angles range from 4–60°. In the second O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one La3+, and one Ru+4.50+ atom.

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Materials Data on K(RuO2)4 by Materials Project

KRu4O8 crystallizes in the tetragonal I4/m space group. The structure is three-dimensional. K1+ is bonded in a body-centered cubic geometry to eight equivalent O2- atoms. All K–O bond lengths are 2.96 Å. Ru+3.75+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing RuO6 octahedra. The corner-sharing octahedral tilt angles are 53°. There are a spread of Ru–O bond distances ranging from 1.95–2.07 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a trigonal planar geometry to three equivalent Ru+3.75+ atoms. In the second O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent K1+ and three equivalent Ru+3.75+ atoms.

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Materials Data on Dy(Zn10Ru)2 by Materials Project

Dy(RuZn10)2 crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Dy is bonded in a 4-coordinate geometry to sixteen Zn atoms. There are four shorter (3.09 Å) and twelve longer (3.15 Å) Dy–Zn bond lengths. Ru is bonded to twelve Zn atoms to form RuZn12 cuboctahedra that share corners with six equivalent RuZn12 cuboctahedra, edges with eighteen equivalent ZnDyZn10Ru cuboctahedra, and faces with six equivalent ZnDyZn10Ru cuboctahedra. There are six shorter (2.53 Å) and six longer (2.77 Å) Ru–Zn bond lengths. There are three inequivalent Zn sites. In the first Zn site, Zn is bonded in a distorted linear geometry to two equivalent Ru and six equivalent Zn atoms. There are two shorter (2.68 Å) and four longer (2.81 Å) Zn–Zn bond lengths. In the second Zn site, Zn is bonded to one Dy, one Ru, and ten Zn atoms to form distorted ZnDyZn10Ru cuboctahedra that share corners with fifteen equivalent ZnDyZn10Ru cuboctahedra, edges with two equivalent ZnDyZn10Ru cuboctahedra, edges with three equivalent RuZn12 cuboctahedra, a faceface with one RuZn12 cuboctahedra, and faces with fifteen equivalent ZnDyZn10Ru cuboctahedra. There are a spread of Zn–Zn bond distances ranging from 2.65–3.04 Å. In the third Zn site, Zn is bonded in a distorted linear geometry to two equivalent Dy and twelve equivalent Zn atoms.

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Materials Data on Ba3NdRu2O9 by Materials Project

Ba3NdRu2O9 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form distorted BaO12 cuboctahedra that share corners with nine BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, faces with three equivalent NdO6 octahedra, and faces with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ba–O bond distances ranging from 2.86–3.34 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent NdO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (2.99 Å) and six longer (3.01 Å) Ba–O bond lengths. Nd3+ is bonded to six equivalent O2- atoms to form NdO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 2°. All Nd–O bond lengths are 2.31 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent NdO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (1.95 Å) and three longer (2.06 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Nd3+, and one Ru+4.50+ atom. In the second O2- site, O2- is bonded to four Ba2+ and two equivalent Ru+4.50+ atoms to form a mixture of distorted face and corner-sharing OBa4Ru2 octahedra. The corner-sharing octahedra tilt angles range from 4–60°.

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Materials Data on In3Ru by Materials Project

RuIn3 crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Ru is bonded in a 8-coordinate geometry to eight In atoms. There are a spread of Ru–In bond distances ranging from 2.68–2.81 Å. There are two inequivalent In sites. In the first In site, In is bonded in a linear geometry to two equivalent Ru atoms. In the second In site, In is bonded in a 1-coordinate geometry to three equivalent Ru atoms.

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Materials Data on Ba3SmRu2O9 by Materials Project

Ba3SmRu2O9 is (Cubic) Perovskite-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with nine BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, faces with three equivalent SmO6 octahedra, and faces with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ba–O bond distances ranging from 2.89–3.24 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent SmO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (2.99 Å) and six longer (3.00 Å) Ba–O bond lengths. Sm3+ is bonded to six equivalent O2- atoms to form SmO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 2°. All Sm–O bond lengths are 2.28 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent SmO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 2°. There are three shorter (1.96 Å) and three longer (2.05 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Sm3+, and one Ru+4.50+ atom. In the second O2- site, O2- is bonded to four Ba2+ and two equivalent Ru+4.50+ atoms to form a mixture of distorted corner and face-sharing OBa4Ru2 octahedra. The corner-sharing octahedra tilt angles range from 4–60°.

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Materials Data on Ba3CeRu2O9 by Materials Project

Ba3CeRu2O9 is (Cubic) Perovskite-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with nine BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, faces with three equivalent CeO6 octahedra, and faces with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 13°. There are a spread of Ba–O bond distances ranging from 2.91–3.20 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent CeO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (2.99 Å) and six longer (3.01 Å) Ba–O bond lengths. Ce3+ is bonded to six equivalent O2- atoms to form CeO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 0°. All Ce–O bond lengths are 2.23 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent CeO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are three shorter (2.00 Å) and three longer (2.04 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Ce3+, and one Ru+4.50+ atom. In the second O2- site, O2- is bonded to four Ba2+ and two equivalent Ru+4.50+ atoms to form a mixture of distorted corner and face-sharing OBa4Ru2 octahedra. The corner-sharing octahedra tilt angles range from 4–60°.

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Materials Data on Ba3TbRu2O9 by Materials Project

Ba3TbRu2O9 is (Cubic) Perovskite-derived structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with nine BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, faces with three equivalent TbO6 octahedra, and faces with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 14°. There are a spread of Ba–O bond distances ranging from 2.91–3.14 Å. In the second Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six equivalent BaO12 cuboctahedra, faces with two equivalent TbO6 octahedra, and faces with six equivalent RuO6 octahedra. There are six shorter (2.98 Å) and six longer (2.99 Å) Ba–O bond lengths. Tb3+ is bonded to six equivalent O2- atoms to form TbO6 octahedra that share corners with six equivalent RuO6 octahedra and faces with eight BaO12 cuboctahedra. The corner-sharing octahedral tilt angles are 1°. All Tb–O bond lengths are 2.24 Å. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent TbO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (1.97 Å) and three longer (2.05 Å) Ru–O bond lengths. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Tb3+, and one Ru+4.50+ atom. In the second O2- site, O2- is bonded in a 6-coordinate geometry to four Ba2+ and two equivalent Ru+4.50+ atoms.

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Materials Data on Y(Zn10Ru)2 by Materials Project

Y(RuZn10)2 crystallizes in the cubic Fd-3m space group. The structure is three-dimensional. Y is bonded in a 4-coordinate geometry to sixteen Zn atoms. There are four shorter (3.09 Å) and twelve longer (3.16 Å) Y–Zn bond lengths. Ru is bonded to twelve Zn atoms to form RuZn12 cuboctahedra that share corners with six equivalent RuZn12 cuboctahedra, edges with eighteen equivalent ZnYZn10Ru cuboctahedra, and faces with six equivalent ZnYZn10Ru cuboctahedra. There are six shorter (2.53 Å) and six longer (2.77 Å) Ru–Zn bond lengths. There are three inequivalent Zn sites. In the first Zn site, Zn is bonded to one Y, one Ru, and ten Zn atoms to form distorted ZnYZn10Ru cuboctahedra that share corners with fifteen equivalent ZnYZn10Ru cuboctahedra, edges with two equivalent ZnYZn10Ru cuboctahedra, edges with three equivalent RuZn12 cuboctahedra, a faceface with one RuZn12 cuboctahedra, and faces with fifteen equivalent ZnYZn10Ru cuboctahedra. There are a spread of Zn–Zn bond distances ranging from 2.66–3.05 Å. In the second Zn site, Zn is bonded in a distorted linear geometry to two equivalent Y and twelve equivalent Zn atoms. In the third Zn site, Zn is bonded in a distorted linear geometry to two equivalent Ru and six equivalent Zn atoms.

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Materials Data on Mg2H4Ru by Materials Project

Mg2RuH4 crystallizes in the orthorhombic Cmcm space group. The structure is three-dimensional. Mg is bonded in a 2-coordinate geometry to eight H atoms. There are a spread of Mg–H bond distances ranging from 2.11–2.43 Å. Ru is bonded in a distorted rectangular see-saw-like geometry to four H atoms. There is two shorter (1.67 Å) and two longer (1.70 Å) Ru–H bond length. There are two inequivalent H sites. In the first H site, H is bonded to four equivalent Mg and one Ru atom to form a mixture of distorted edge, face, and corner-sharing HMg4Ru square pyramids. In the second H site, H is bonded to four equivalent Mg and one Ru atom to form a mixture of distorted edge, face, and corner-sharing HMg4Ru square pyramids.

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Materials Data on Ge2RuC4(Cl3O2)2 by Materials Project

Ru(CO)4(GeCl3)2 crystallizes in the monoclinic P2_1 space group. The structure is zero-dimensional and consists of eight trichlorogermane molecules and four Ru(CO)4 clusters. In each Ru(CO)4 cluster, Ru6+ is bonded in a rectangular see-saw-like geometry to four C atoms. There is one shorter (1.96 Å) and three longer (1.97 Å) Ru–C bond length. There are four inequivalent C sites. In the first C site, C is bonded in a linear geometry to one Ru6+ and one O2- atom. The C–O bond length is 1.15 Å. In the second C site, C is bonded in a distorted linear geometry to one Ru6+ and one O2- atom. The C–O bond length is 1.15 Å. In the third C site, C is bonded in a distorted linear geometry to one Ru6+ and one O2- atom. The C–O bond length is 1.15 Å. In the fourth C site, C is bonded in a linear geometry to one Ru6+ and one O2- atom. The C–O bond length is 1.15 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C atom. In the fourth O2- site, O2- is bonded in a single-bond geometry to one C atom.

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Materials Data on SbRu2C6Cl7O6 by Materials Project

(RuC3O3Cl2)2SbCl3 crystallizes in the monoclinic P2_1/c space group. The structure is zero-dimensional and consists of four antimony trichloride molecules and four RuC3O3Cl2 clusters. In two of the RuC3O3Cl2 clusters, Ru3+ is bonded to three C+2.67+ and three Cl1- atoms to form distorted edge-sharing RuC3Cl3 octahedra. There is one shorter (1.90 Å) and two longer (1.91 Å) Ru–C bond length. There are a spread of Ru–Cl bond distances ranging from 2.43–2.49 Å. There are three inequivalent C+2.67+ sites. In the first C+2.67+ site, C+2.67+ is bonded in a single-bond geometry to one Ru3+ and one O2- atom. The C–O bond length is 1.15 Å. In the second C+2.67+ site, C+2.67+ is bonded in a single-bond geometry to one Ru3+ and one O2- atom. The C–O bond length is 1.15 Å. In the third C+2.67+ site, C+2.67+ is bonded in a single-bond geometry to one Ru3+ and one O2- atom. The C–O bond length is 1.15 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a distorted single-bond geometry to one Ru3+ atom. In the second Cl1- site, Cl1- is bonded in a distorted L-shaped geometry to two equivalent Ru3+ atoms. In two of the RuC3O3Cl2 clusters, Ru3+ is bonded to three C+2.67+ and three Cl1- atoms to form distorted edge-sharing RuC3Cl3 octahedra. There are a spread of Ru–C bond distances ranging from 1.89–1.92 Å. There are one shorter (2.42 Å) and two longer (2.49 Å) Ru–Cl bond lengths. There are three inequivalent C+2.67+ sites. In the first C+2.67+ site, C+2.67+ is bonded in a single-bond geometry to one Ru3+ and one O2- atom. The C–O bond length is 1.15 Å. In the second C+2.67+ site, C+2.67+ is bonded in a single-bond geometry to one Ru3+ and one O2- atom. The C–O bond length is 1.15 Å. In the third C+2.67+ site, C+2.67+ is bonded in a single-bond geometry to one Ru3+ and one O2- atom. The C–O bond length is 1.15 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the second O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. In the third O2- site, O2- is bonded in a single-bond geometry to one C+2.67+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in an L-shaped geometry to two equivalent Ru3+ atoms. In the second Cl1- site, Cl1- is bonded in a single-bond geometry to one Ru3+ atom.

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Materials Data on Ga3Ru by Materials Project

RuGa3 crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. Ru is bonded in a 8-coordinate geometry to eight Ga atoms. There are a spread of Ru–Ga bond distances ranging from 2.45–2.60 Å. There are two inequivalent Ga sites. In the first Ga site, Ga is bonded in a linear geometry to two equivalent Ru atoms. In the second Ga site, Ga is bonded in a 1-coordinate geometry to three equivalent Ru atoms.

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Materials Data on In3Ru by Materials Project

RuIn3 crystallizes in the tetragonal P-4n2 space group. The structure is three-dimensional. Ru is bonded in a 8-coordinate geometry to eight In atoms. There are a spread of Ru–In bond distances ranging from 2.69–2.83 Å. There are two inequivalent In sites. In the first In site, In is bonded in a linear geometry to two equivalent Ru atoms. In the second In site, In is bonded in a 1-coordinate geometry to three equivalent Ru atoms.

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Materials Data on Ru4Pb4O13 by Materials Project

Ru4Pb4O13 crystallizes in the cubic F-43m space group. The structure is three-dimensional. Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with six equivalent RuO6 octahedra and edges with six equivalent PbO7 hexagonal pyramids. The corner-sharing octahedra tilt angles range from 43–45°. All Ru–O bond lengths are 1.98 Å. Pb2+ is bonded to seven O2- atoms to form distorted PbO7 hexagonal pyramids that share corners with three equivalent PbO7 hexagonal pyramids, edges with three equivalent PbO7 hexagonal pyramids, and edges with six equivalent RuO6 octahedra. There are a spread of Pb–O bond distances ranging from 2.28–2.61 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 4-coordinate geometry to two equivalent Ru+4.50+ and two equivalent Pb2+ atoms. In the second O2- site, O2- is bonded in a 2-coordinate geometry to two equivalent Ru+4.50+ and two equivalent Pb2+ atoms. In the third O2- site, O2- is bonded in a tetrahedral geometry to four equivalent Pb2+ atoms.

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