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At least 1,675 records · Page 93

Materials Data on Ti2FeRu by Materials Project

Ti2RuFe 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 four equivalent Ru and four equivalent Fe atoms. All Ti–Ru bond lengths are 2.62 Å. All Ti–Fe bond lengths are 2.62 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Ti atoms. Fe is bonded in a distorted body-centered cubic geometry to eight equivalent Ti atoms.

36 MATERIALS SCIENCE↗

Materials Data on Nb2OsRu by Materials Project

Nb2OsRu crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Nb2OsRu ribbons oriented in the (1, 0, 0) direction. Nb is bonded in a linear geometry to one Os and one Ru atom. The Nb–Os bond length is 2.26 Å. The Nb–Ru bond length is 2.22 Å. Os is bonded in a linear geometry to two equivalent Nb atoms. Ru is bonded in a linear geometry to two equivalent Nb atoms.

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Materials Data on Eu(BRu)4 by Materials Project

Eu(RuB)4 crystallizes in the tetragonal I4_1/acd space group. The structure is three-dimensional. Eu2+ is bonded in a 12-coordinate geometry to twelve equivalent B3- atoms. There are a spread of Eu–B bond distances ranging from 2.96–3.25 Å. Ru+2.50+ is bonded to five equivalent B3- atoms to form a mixture of distorted edge and corner-sharing RuB5 trigonal bipyramids. There are a spread of Ru–B bond distances ranging from 2.15–2.31 Å. B3- is bonded in a 6-coordinate geometry to three equivalent Eu2+, five equivalent Ru+2.50+, and one B3- atom. The B–B bond length is 1.80 Å.

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Materials Data on Nd2ZnRu by Materials Project

Nd2RuZn is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Nd is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Zn atoms. All Nd–Ru bond lengths are 3.12 Å. All Nd–Zn bond lengths are 3.12 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Nd atoms. Zn is bonded in a body-centered cubic geometry to eight equivalent Nd atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sc2OsRu by Materials Project

Sc2OsRu crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Sc2OsRu ribbons oriented in the (1, 0, 0) direction. Sc is bonded in a linear geometry to one Os and one Ru atom. The Sc–Os bond length is 2.37 Å. The Sc–Ru bond length is 2.34 Å. Os is bonded in a linear geometry to two equivalent Sc atoms. Ru is bonded in a linear geometry to two equivalent Sc atoms.

36 MATERIALS SCIENCE↗

Materials Data on V2RuW by Materials Project

V2WRu crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two V2WRu ribbons oriented in the (1, 0, 0) direction. V is bonded in a linear geometry to one W and one Ru atom. The V–W bond length is 2.26 Å. The V–Ru bond length is 2.20 Å. W is bonded in a linear geometry to two equivalent V atoms. Ru is bonded in a linear geometry to two equivalent V atoms.

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Materials Data on H17RuN6Cl3O2 by Materials Project

RuN4H7O2Cl(NH3)2H2(HCl)2 crystallizes in the orthorhombic Pna2_1 space group. The structure is zero-dimensional and consists of eight ammonia molecules, eight hydrochloric acid molecules, four hydrogen molecules, and four RuN4H7O2Cl clusters. In each RuN4H7O2Cl cluster, Ru2+ is bonded in a trigonal bipyramidal geometry to two N2-, two O2-, and one Cl1- atom. There is one shorter (1.86 Å) and one longer (1.87 Å) Ru–N bond length. There is one shorter (1.90 Å) and one longer (2.06 Å) Ru–O bond length. The Ru–Cl bond length is 2.38 Å. There are four inequivalent N2- sites. In the first N2- site, N2- is bonded in a bent 120 degrees geometry to one N2- and two H1+ atoms. The N–N bond length is 1.32 Å. There is one shorter (1.02 Å) and one longer (1.03 Å) N–H bond length. In the second N2- site, N2- is bonded in a distorted trigonal planar geometry to one Ru2+ and two H1+ atoms. Both N–H bond lengths are 1.02 Å. In the third N2- site, N2- is bonded in a distorted trigonal planar geometry to one Ru2+ and two H1+ atoms. There is one shorter (1.02 Å) and one longer (1.03 Å) N–H bond length. In the fourth N2- site, N2- is bonded in a distorted water-like geometry to one N2- and one O2- atom. The N–O bond length is 1.26 Å. There are seven inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one O2- atom. The H–O bond length is 0.98 Å. In the second H1+ site, H1+ is bonded in a single-bond geometry to one N2- atom. In the third H1+ site, H1+ is bonded in a single-bond geometry to one N2- atom. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one N2- atom. In the fifth H1+ site, H1+ is bonded in a single-bond geometry to one N2- atom. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one N2- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one N2- atom. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted water-like geometry to one Ru2+ and one H1+ atom. In the second O2- site, O2- is bonded in a distorted bent 120 degrees geometry to one Ru2+ and one N2- atom. Cl1- is bonded in a single-bond geometry to one Ru2+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Ta3Ru by Materials Project

Ta3Ru crystallizes in the orthorhombic Cmmm space group. The structure is three-dimensional. there are two inequivalent Ta sites. In the first Ta site, Ta is bonded in a 2-coordinate geometry to two equivalent Ta and two equivalent Ru atoms. Both Ta–Ta bond lengths are 2.86 Å. Both Ta–Ru bond lengths are 2.67 Å. In the second Ta site, Ta is bonded in a distorted body-centered cubic geometry to eight Ta atoms. All Ta–Ta bond lengths are 2.88 Å. Ru is bonded in a 4-coordinate geometry to four equivalent Ta atoms.

36 MATERIALS SCIENCE↗

Materials Data on Te16(Mo3Ru)3 by Materials Project

Te16(Mo3Ru)3 crystallizes in the triclinic P1 space group. The structure is three-dimensional. there are nine inequivalent Mo+2.89+ sites. In the first Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.71–2.88 Å. In the second Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, edges with two RuTe5 square pyramids, and edges with three MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.72–2.84 Å. In the third Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share corners with two MoTe5 square pyramids, corners with two RuTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.76–2.88 Å. In the fourth Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share corners with four MoTe5 square pyramids, edges with two RuTe5 square pyramids, and edges with three MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.72–2.85 Å. In the fifth Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.74–2.88 Å. In the sixth Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, edges with two RuTe5 square pyramids, and edges with three MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.73–2.84 Å. In the seventh Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.73–2.86 Å. In the eighth Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share corners with two MoTe5 square pyramids, corners with two RuTe5 square pyramids, edges with two RuTe5 square pyramids, and edges with three MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.71–2.88 Å. In the ninth Mo+2.89+ site, Mo+2.89+ is bonded to five Te2- atoms to form MoTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Mo–Te bond distances ranging from 2.72–2.88 Å. There are three inequivalent Ru2+ sites. In the first Ru2+ site, Ru2+ is bonded to five Te2- atoms to form RuTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Ru–Te bond distances ranging from 2.66–2.83 Å. In the second Ru2+ site, Ru2+ is bonded to five Te2- atoms to form RuTe5 square pyramids that share corners with four MoTe5 square pyramids and edges with five MoTe5 square pyramids. There are a spread of Ru–Te bond distances ranging from 2.68–2.81 Å. In the third Ru2+ site, Ru2+ is bonded to five Te2- atoms to form RuTe5 square pyramids that share a cornercorner with one RuTe5 square pyramid, corners with three MoTe5 square pyramids, an edgeedge with one RuTe5 square pyramid, and edges with four MoTe5 square pyramids. There are a spread of Ru–Te bond distances ranging from 2.65–2.82 Å. There are sixteen inequivalent Te2- sites. In the first Te2- site, Te2- is bonded in a 6-coordinate geometry to one Mo+2.89+ and two Ru2+ atoms. In the second Te2- site, Te2- is bonded in a 6-coordinate geometry to two Mo+2.89+ and one Ru2+ atom. In the third Te2- site, Te2- is bonded in a 6-coordinate geometry to three Mo+2.89+ atoms. In the fourth Te2- site, Te2- is bonded in a 6-coordinate geometry to three Mo+2.89+ atoms. In the fifth Te2- site, Te2- is bonded in a distorted rectangular see-saw-like geometry to two Mo+2.89+ and two Ru2+ atoms. In the sixth Te2- site, Te2- is bonded in a distorted rectangular see-saw-like geometry to three Mo+2.89+ and one Ru2+ atom. In the seventh Te2- site, Te2- is bonded in a distorted rectangular see-saw-like geometry to three Mo+2.89+ and one Ru2+ atom. In the eighth Te2- site, Te2- is bonded in a 4-coordinate geometry to four Mo+2.89+ atoms. In the ninth Te2- site, Te2- is bonded in a 4-coordinate geometry to three Mo+2.89+ and one Ru2+ atom. In the tenth Te2- site, Te2- is bonded in a 4-coordinate geometry to three Mo+2.89+ and one Ru2+ atom. In the eleventh Te2- site, Te2- is bonded in a 4-coordinate geometry to three Mo+2.89+ and one Ru2+ atom. In the twelfth Te2- site, Te2- is bonded in a 4-coordinate geometry to three Mo+2.89+ and one Ru2+ atom. In the thirteenth Te2- site, Te2- is bonded in a 4-coordinate geometry to two Mo+2.89+ and two Ru2+ atoms. In the fourteenth Te2- site, Te2- is bonded in a 4-coordinate geometry to three Mo+2.89+ and one Ru2+ atom. In the fifteenth Te2- site, Te2- is bonded in a 4-coordinate geometry to three Mo+2.89+ and one Ru2+ atom. In the sixteenth Te2- site, Te2- is bonded in a 4-coordinate geometry to four Mo+2.89+ atoms.

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Materials Data on Ti2CoRu by Materials Project

Ti2RuCo crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Ti2RuCo ribbons oriented in the (1, 0, 0) direction. Ti is bonded in a linear geometry to one Ru and one Co atom. The Ti–Ru bond length is 2.10 Å. The Ti–Co bond length is 2.01 Å. Ru is bonded in a linear geometry to two equivalent Ti atoms. Co is bonded in a linear geometry to two equivalent Ti atoms.

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Materials Data on Er2RuAu by Materials Project

Er2RuAu is Heusler structured and crystallizes in the cubic Fm-3m space group. The structure is three-dimensional. Er is bonded in a body-centered cubic geometry to four equivalent Ru and four equivalent Au atoms. All Er–Ru bond lengths are 3.01 Å. All Er–Au bond lengths are 3.01 Å. Ru is bonded in a body-centered cubic geometry to eight equivalent Er atoms. Au is bonded in a body-centered cubic geometry to eight equivalent Er atoms.

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Materials Data on MgZn2Ru by Materials Project

MgRuZn2 crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two MgRuZn2 ribbons oriented in the (1, 0, 0) direction. Mg is bonded in a linear geometry to two equivalent Zn atoms. Both Mg–Zn bond lengths are 2.83 Å. Ru is bonded in a linear geometry to two equivalent Zn atoms. Both Ru–Zn bond lengths are 2.48 Å. Zn is bonded in a linear geometry to one Mg and one Ru atom.

36 MATERIALS SCIENCE↗

Materials Data on Zr2TcRu by Materials Project

Zr2TcRu crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Zr2TcRu ribbons oriented in the (1, 0, 0) direction. Zr is bonded in a linear geometry to one Tc and one Ru atom. The Zr–Tc bond length is 2.31 Å. The Zr–Ru bond length is 2.29 Å. Tc is bonded in a linear geometry to two equivalent Zr atoms. Ru is bonded in a linear geometry to two equivalent Zr atoms.

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Materials Data on Rb3Ru2N(Cl4O)2 by Materials Project

Rb3Ru2N(OCl4)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 8-coordinate geometry to eight Cl1- atoms. There are a spread of Rb–Cl bond distances ranging from 3.33–3.46 Å. In the second Rb1+ site, Rb1+ is bonded in a body-centered cubic geometry to eight Cl1- atoms. There are four shorter (3.40 Å) and four longer (3.42 Å) Rb–Cl bond lengths. Ru6+ is bonded to one N3-, one O2-, and four Cl1- atoms to form distorted corner-sharing RuNCl4O octahedra. The corner-sharing octahedral tilt angles are 0°. The Ru–N bond length is 1.88 Å. The Ru–O bond length is 1.73 Å. There are two shorter (2.40 Å) and two longer (2.41 Å) Ru–Cl bond lengths. N3- is bonded in a linear geometry to two equivalent Ru6+ atoms. O2- is bonded in a single-bond geometry to one Ru6+ atom. There are two inequivalent Cl1- sites. In the first Cl1- site, Cl1- is bonded in a 4-coordinate geometry to three Rb1+ and one Ru6+ atom. In the second Cl1- site, Cl1- is bonded in a 1-coordinate geometry to three Rb1+ and one Ru6+ atom.

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Materials Data on Y2AlRu by Materials Project

Y2RuAl crystallizes in the orthorhombic Immm space group. The structure is one-dimensional and consists of two Y2RuAl ribbons oriented in the (1, 0, 0) direction. Y is bonded in a linear geometry to one Ru and one Al atom. The Y–Ru bond length is 2.34 Å. The Y–Al bond length is 2.94 Å. Ru is bonded in a linear geometry to two equivalent Y atoms. Al is bonded in a linear geometry to two equivalent Y atoms.

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Stabilizing Reversible Oxygen Redox Chemistry in Layered Oxides for Sodium‐Ion Batteries

Abstract Triggering oxygen‐related activity is demonstrated as a promising strategy to effectively boost energy density of layered cathodes for sodium‐ion batteries. However, irreversible lattice oxygen loss will induce detrimental structure distortion, resulting in voltage decay and cycle degradation. Herein, a layered structure P2‐type Na 0.66 Li 0.22 Ru 0.78 O 2 cathode is designed, delivering reversible oxygen‐related and Ru‐based redox chemistry simultaneously. Benefiting from the combination of strong Ru 4d‐O 2p covalency and stable Li location within the transition metal layer, reversible anionic/cationic redox chemistry is achieved successfully, which is proved by systematic bulk/surface analysis by in/ex situ spectroscopy (operando Raman and hard X‐ray absorption spectroscopy, etc.). Moreover, the robust structure and reversible phase transition evolution revealed by operando X‐ray diffraction further establish a high degree reversible (de)intercalation processes (≈150 mAh g −1 , reversible capacity) and long‐term cycling (average capacity drop of 0.018%, 500 cycles).

Cao, Xin↗

Atomically Precise Crystalline Materials Based on Kinetically Inert Metal Ions via Reticular Mechanopolymerization

Abstract Atomistic control of the coordination environment of lattice ions and the distribution of metal sites within crystalline mixed‐metal coordination polymers remain significant synthetic challenges. Herein is reported the mechanochemical synthesis of a reticular family of crystalline heterobimetallic metal–organic frameworks (MOFs) is now achieved by polymerization of molecular Ru 2 [II,III] complexes, featuring unprotected carboxylic acid substituents, with Cu(OAc) 2 . The resulting crystalline heterobimetallic MOFs are solid solutions of Ru 2 and Cu 2 sites housed within [M 3 L 2 ] phases. The developed mechanochemical strategy is modular and allows for systematic control of the primary coordination sphere of the Ru 2 sites within an isoreticular family of materials. This strategy is anticipated to provide a rational approach to atomically precise mixed‐metal materials.

Gao, Wen‐Yang↗