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At least 487 records · Page 27

Materials Data on Ba7Ru4Cl2O15 by Materials Project

Ba7Ru4O15Cl2 crystallizes in the trigonal R-3m space group. The structure is three-dimensional. there are four inequivalent Ba2+ sites. In the first Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with nine equivalent BaO12 cuboctahedra, faces with three equivalent BaO12 cuboctahedra, and faces with seven RuO6 octahedra. There are a spread of Ba–O bond distances ranging from 2.92–2.99 Å. In the second Ba2+ site, Ba2+ is bonded in a 10-coordinate geometry to nine O2- and one Cl1- atom. There are three shorter (2.72 Å) and six longer (2.97 Å) Ba–O bond lengths. The Ba–Cl bond length is 3.16 Å. In the third Ba2+ site, Ba2+ is bonded in a 7-coordinate geometry to three equivalent O2- and four equivalent Cl1- atoms. All Ba–O bond lengths are 2.57 Å. There are one shorter (3.22 Å) and three longer (3.51 Å) Ba–Cl bond lengths. In the fourth Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with six equivalent BaO12 cuboctahedra, corners with six equivalent RuO6 octahedra, faces with six equivalent BaO12 cuboctahedra, and faces with six equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 10°. There are six shorter (2.94 Å) and six longer (3.01 Å) Ba–O bond lengths. There are two inequivalent Ru+4.50+ sites. In the first Ru+4.50+ site, Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, faces with three equivalent BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. There are three shorter (1.91 Å) and three longer (2.11 Å) Ru–O bond lengths. In the second Ru+4.50+ site, Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 0°. All Ru–O bond lengths are 2.02 Å. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 6-coordinate geometry to four Ba2+ and two Ru+4.50+ atoms. In the second O2- site, O2- is bonded in a 5-coordinate geometry to four Ba2+ and one Ru+4.50+ atom. In the third O2- site, O2- is bonded in a distorted linear geometry to four Ba2+ and two equivalent Ru+4.50+ atoms. Cl1- is bonded to five Ba2+ atoms to form a mixture of distorted edge and corner-sharing ClBa5 trigonal bipyramids.

36 MATERIALS SCIENCE↗

Materials Data on Gd5(RuO7)2 by Materials Project

Gd5(RuO7)2 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are two inequivalent Gd sites. In the first Gd site, Gd is bonded to seven O atoms to form distorted GdO7 pentagonal bipyramids that share corners with two RuO6 octahedra, corners with three equivalent GdO7 pentagonal bipyramids, edges with two RuO6 octahedra, and edges with two equivalent GdO7 pentagonal bipyramids. The corner-sharing octahedra tilt angles range from 30–37°. There are a spread of Gd–O bond distances ranging from 2.21–2.51 Å. In the second Gd site, Gd is bonded in a distorted square co-planar geometry to eight O atoms. There are four shorter (2.25 Å) and four longer (2.82 Å) Gd–O bond lengths. There are two inequivalent Ru sites. In the first Ru site, Ru is bonded to six O atoms to form RuO6 octahedra that share corners with two equivalent RuO6 octahedra, corners with four equivalent GdO7 pentagonal bipyramids, and edges with four equivalent GdO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 39°. There is four shorter (1.91 Å) and two longer (2.02 Å) Ru–O bond length. In the second Ru site, Ru is bonded to six O atoms to form RuO6 octahedra that share corners with two equivalent RuO6 octahedra, corners with four equivalent GdO7 pentagonal bipyramids, and edges with four equivalent GdO7 pentagonal bipyramids. The corner-sharing octahedral tilt angles are 39°. There is four shorter (1.90 Å) and two longer (2.00 Å) Ru–O bond length. There are four inequivalent O sites. In the first O site, O is bonded in a trigonal planar geometry to three Gd atoms. In the second O site, O is bonded in a 4-coordinate geometry to three Gd and one Ru atom. In the third O site, O is bonded in a 3-coordinate geometry to two equivalent Gd and one Ru atom. In the fourth O site, O is bonded to two equivalent Gd and two Ru atoms to form distorted corner-sharing OGd2Ru2 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Ru3W3C2 by Materials Project

W3Ru3C2 is H-Phase-like structured and crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. there are two inequivalent W sites. In the first W site, W is bonded to nine W and three equivalent Ru atoms to form WRu3W9 cuboctahedra that share corners with nine equivalent WRu3W9 cuboctahedra, corners with six equivalent CRu6 octahedra, edges with fifteen WRu3W9 cuboctahedra, faces with twelve WRu3W9 cuboctahedra, and a faceface with one CRu6 octahedra. The corner-sharing octahedral tilt angles are 44°. There are six shorter (2.86 Å) and three longer (2.90 Å) W–W bond lengths. All W–Ru bond lengths are 2.76 Å. In the second W site, W is bonded to twelve W atoms to form WW12 cuboctahedra that share corners with six equivalent WW12 cuboctahedra, edges with eighteen WRu3W9 cuboctahedra, and faces with eighteen WRu3W9 cuboctahedra. All W–W bond lengths are 2.86 Å. There are two inequivalent Ru sites. In the first Ru site, Ru is bonded in a 3-coordinate geometry to three equivalent W and three equivalent C atoms. All Ru–C bond lengths are 2.06 Å. In the second Ru site, Ru is bonded to six equivalent C atoms to form edge-sharing RuC6 octahedra. All Ru–C bond lengths are 2.20 Å. C is bonded to six Ru atoms to form CRu6 octahedra that share corners with six equivalent WRu3W9 cuboctahedra, corners with three equivalent CRu6 octahedra, edges with nine equivalent CRu6 octahedra, and a faceface with one WRu3W9 cuboctahedra. The corner-sharing octahedral tilt angles are 0°.

36 MATERIALS SCIENCE↗

Materials Data on Al3Ru by Materials Project

Al3Ru is Uranium Silicide-like structured and crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. there are two inequivalent Ru sites. In the first Ru site, Ru is bonded to twelve Al atoms to form RuAl12 cuboctahedra that share corners with six equivalent RuAl12 cuboctahedra, corners with twelve equivalent AlAl8Ru4 cuboctahedra, edges with eighteen AlAl8Ru4 cuboctahedra, faces with eight RuAl12 cuboctahedra, and faces with twelve AlAl8Ru4 cuboctahedra. There are six shorter (2.72 Å) and six longer (2.73 Å) Ru–Al bond lengths. In the second Ru site, Ru is bonded to twelve Al atoms to form RuAl12 cuboctahedra that share corners with twelve equivalent RuAl12 cuboctahedra, edges with twenty-four AlAl8Ru4 cuboctahedra, faces with six equivalent RuAl12 cuboctahedra, and faces with twelve AlAl8Ru4 cuboctahedra. There are six shorter (2.73 Å) and six longer (2.74 Å) Ru–Al bond lengths. There are three inequivalent Al sites. In the first Al site, Al is bonded to four Ru and eight Al atoms to form distorted AlAl8Ru4 cuboctahedra that share corners with four equivalent RuAl12 cuboctahedra, corners with fourteen equivalent AlAl8Ru4 cuboctahedra, edges with six RuAl12 cuboctahedra, edges with twelve AlAl8Ru4 cuboctahedra, faces with four RuAl12 cuboctahedra, and faces with sixteen AlAl8Ru4 cuboctahedra. There are four shorter (2.73 Å) and four longer (2.74 Å) Al–Al bond lengths. In the second Al site, Al is bonded to four Ru and eight Al atoms to form distorted AlAl8Ru4 cuboctahedra that share corners with twelve equivalent AlAl8Ru4 cuboctahedra, edges with eight RuAl12 cuboctahedra, edges with sixteen AlAl8Ru4 cuboctahedra, faces with four RuAl12 cuboctahedra, and faces with fourteen AlAl8Ru4 cuboctahedra. There are two shorter (2.68 Å) and two longer (2.78 Å) Al–Al bond lengths. In the third Al site, Al is bonded to four Ru and eight Al atoms to form distorted AlAl8Ru4 cuboctahedra that share corners with twelve AlAl8Ru4 cuboctahedra, edges with eight RuAl12 cuboctahedra, edges with sixteen AlAl8Ru4 cuboctahedra, faces with four RuAl12 cuboctahedra, and faces with fourteen AlAl8Ru4 cuboctahedra.

36 MATERIALS SCIENCE↗

Materials Data on Ba3FeRu2O9 by Materials Project

Ba3FeRu2O9 is (Cubic) Perovskite-derived structured and crystallizes in the hexagonal P6_3mc space group. The structure is three-dimensional. there are three 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 FeO6 octahedra, faces with seven BaO12 cuboctahedra, a faceface with one FeO6 octahedra, and faces with six RuO6 octahedra. The corner-sharing octahedral tilt angles are 7°. There are a spread of Ba–O bond distances ranging from 2.84–2.99 Å. In the second 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 FeO6 octahedra, and faces with four RuO6 octahedra. The corner-sharing octahedral tilt angles are 11°. There are nine shorter (2.91 Å) and three longer (2.99 Å) Ba–O bond lengths. In the third Ba2+ site, Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with twelve BaO12 cuboctahedra, faces with six BaO12 cuboctahedra, faces with three equivalent FeO6 octahedra, and faces with five RuO6 octahedra. There are a spread of Ba–O bond distances ranging from 2.89–2.96 Å. There are two inequivalent Ru+4.50+ sites. In the first Ru+4.50+ site, Ru+4.50+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three equivalent RuO6 octahedra, corners with three equivalent FeO6 octahedra, and faces with eight BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 1–5°. There are three shorter (1.99 Å) and three longer (2.01 Å) Ru–O bond lengths. In the second Ru+4.50+ site, 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 RuO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one FeO6 octahedra. The corner-sharing octahedral tilt angles are 1°. There are three shorter (1.99 Å) and three longer (2.01 Å) Ru–O bond lengths. Fe3+ is bonded to six O2- atoms to form FeO6 octahedra that share corners with three equivalent BaO12 cuboctahedra, corners with three equivalent RuO6 octahedra, faces with seven BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 5°. There are three shorter (1.99 Å) and three longer (2.11 Å) Fe–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four Ba2+, one Ru+4.50+, and one Fe3+ atom to form a mixture of distorted corner and face-sharing OBa4FeRu octahedra. The corner-sharing octahedra tilt angles range from 7–60°. In the second O2- site, O2- is bonded in a distorted linear geometry to four Ba2+ and two Ru+4.50+ atoms. In the third O2- site, O2- is bonded in a distorted linear geometry to four Ba2+, one Ru+4.50+, and one Fe3+ atom.

36 MATERIALS SCIENCE↗

Materials Data on BaCuRu5O11 by Materials Project

BaRu5CuO11 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with six equivalent BaO12 cuboctahedra, edges with six equivalent RuO6 octahedra, edges with three equivalent CuO5 trigonal bipyramids, and faces with six equivalent RuO6 octahedra. There are six shorter (2.92 Å) and six longer (2.98 Å) Ba–O bond lengths. There are two inequivalent Ru+3.80+ sites. In the first Ru+3.80+ site, Ru+3.80+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with six equivalent RuO6 octahedra, corners with three equivalent CuO5 trigonal bipyramids, faces with three equivalent BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 51°. There are three shorter (2.02 Å) and three longer (2.04 Å) Ru–O bond lengths. In the second Ru+3.80+ site, Ru+3.80+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with four equivalent RuO6 octahedra, corners with two equivalent CuO5 trigonal bipyramids, edges with two equivalent BaO12 cuboctahedra, and edges with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 51°. There are four shorter (2.04 Å) and two longer (2.07 Å) Ru–O bond lengths. Cu1+ is bonded to five O2- atoms to form CuO5 trigonal bipyramids that share corners with twelve RuO6 octahedra and edges with three equivalent BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 42–56°. There are three shorter (1.91 Å) and two longer (2.35 Å) Cu–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a 5-coordinate geometry to two equivalent Ba2+, two equivalent Ru+3.80+, and one Cu1+ atom. In the second O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to three equivalent Ru+3.80+ and one Cu1+ atom. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+ and three Ru+3.80+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on USbRu by Materials Project

URuSb crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. U is bonded in a 11-coordinate geometry to five Ru and six equivalent Sb atoms. There are four shorter (2.99 Å) and one longer (3.06 Å) U–Ru bond lengths. There are two shorter (3.15 Å) and four longer (3.34 Å) U–Sb bond lengths. There are two inequivalent Ru sites. In the first Ru site, Ru is bonded in a 9-coordinate geometry to three equivalent U and six equivalent Sb atoms. All Ru–Sb bond lengths are 2.76 Å. In the second Ru site, Ru is bonded in a 9-coordinate geometry to six equivalent U and three equivalent Sb atoms. All Ru–Sb bond lengths are 2.79 Å. Sb is bonded in a 10-coordinate geometry to six equivalent U and four Ru atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sc4Ge6Ru7 by Materials Project

Sc4Ru7Ge6 crystallizes in the cubic Im-3m space group. The structure is three-dimensional. Sc is bonded to six equivalent Ru and six equivalent Ge atoms to form ScGe6Ru6 cuboctahedra that share corners with twelve equivalent ScGe6Ru6 cuboctahedra, faces with six equivalent ScGe6Ru6 cuboctahedra, and faces with two equivalent RuGe6 octahedra. All Sc–Ru bond lengths are 2.89 Å. All Sc–Ge bond lengths are 2.93 Å. There are two inequivalent Ru sites. In the first Ru site, Ru is bonded to six equivalent Ge atoms to form RuGe6 octahedra that share faces with eight equivalent ScGe6Ru6 cuboctahedra. All Ru–Ge bond lengths are 2.52 Å. In the second Ru site, Ru is bonded in a 12-coordinate geometry to four equivalent Sc and four equivalent Ge atoms. All Ru–Ge bond lengths are 2.57 Å. Ge is bonded in a 9-coordinate geometry to four equivalent Sc and five Ru atoms.

36 MATERIALS SCIENCE↗

Materials Data on BaLiRu5O11 by Materials Project

LiBaRu5O11 crystallizes in the hexagonal P6_3/mmc space group. The structure is three-dimensional. Li1+ is bonded to five O2- atoms to form LiO5 trigonal bipyramids that share corners with twelve RuO6 octahedra and edges with three equivalent BaO12 cuboctahedra. The corner-sharing octahedra tilt angles range from 40–56°. There are three shorter (1.88 Å) and two longer (2.35 Å) Li–O bond lengths. Ba2+ is bonded to twelve O2- atoms to form BaO12 cuboctahedra that share corners with six equivalent BaO12 cuboctahedra, edges with six equivalent RuO6 octahedra, edges with three equivalent LiO5 trigonal bipyramids, and faces with six equivalent RuO6 octahedra. There are six shorter (2.92 Å) and six longer (2.95 Å) Ba–O bond lengths. There are two inequivalent Ru+3.80+ sites. In the first Ru+3.80+ site, Ru+3.80+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with four equivalent RuO6 octahedra, corners with two equivalent LiO5 trigonal bipyramids, edges with two equivalent BaO12 cuboctahedra, and edges with four equivalent RuO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are four shorter (2.03 Å) and two longer (2.06 Å) Ru–O bond lengths. In the second Ru+3.80+ site, Ru+3.80+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with six equivalent RuO6 octahedra, corners with three equivalent LiO5 trigonal bipyramids, faces with three equivalent BaO12 cuboctahedra, and a faceface with one RuO6 octahedra. The corner-sharing octahedral tilt angles are 50°. There are three shorter (2.00 Å) and three longer (2.03 Å) Ru–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to one Li1+ and three equivalent Ru+3.80+ atoms. In the second O2- site, O2- is bonded in a 5-coordinate geometry to one Li1+, two equivalent Ba2+, and two equivalent Ru+3.80+ atoms. In the third O2- site, O2- is bonded in a 4-coordinate geometry to one Ba2+ and three Ru+3.80+ atoms.

36 MATERIALS SCIENCE↗

Plastic-waste hydrogenolysis over two-dimensional MXene-supported ruthenium catalysts with tunable interlayer spacing

The hydrogenolysis of plastics is limited by active-site inaccessibility and inefficient mass transport of bulky polymer chains. To overcome these challenges, this work developed two-dimensional MXene-supported Ru (Ru@MXene) catalysts. Lyophilization of a solution containing dispersed MXene sheets and Ru precursors enabled the confinement of Ru species within the MXene interlayers, which act as pillars to expand the interlayer spacing. Building on this, a silica-pillared MXene-supported Ru (Ru@P-MXene) with even larger interlayer spacing exhibited a reaction rate of 914.9 g C5–C35 g Ru –1 h –1 for the hydrogenolysis of low-density polyethylene (LDPE) into valuable liquid chemicals (e.g., C 5 –C 35 ). A comparison of product yields between Ru@P-MXene and Ru@MXene suggests that elongated Ru particles confined within the MXene support expose their side facets for the reaction. In conclusion, this work demonstrates a new application of MXene in thermochemical catalysis, offering a solution to the challenges of active-site accessibility, mass transport, and reaction confinement in chemical plastic upcycling.

2D materials↗

Proton-Coupled Electron Transfer in a Ruthenium(II) Bipyrimidine Complex in Its Ground and Excited Electronic States

In this work, proton-coupled electron transfer (PCET) was studied for the ground and excited electronic states of a [Ru(terpy)(bpm)(OH 2 )(PF 6 ) 2 ] complex, Ru-bpm. Cyclic voltammetry measurements show that the Ru(II)-aqua moiety undergoes PCET to form a Ru(IV)-oxo moiety in the anodic region, while the bpm ligand undergoes PCET to form bpmH 2 in the cathodic region. The photophysical behavior of Ru-bpm was studied using steady-state and femtosecond transient UV–vis absorption spectroscopy, coupled with density functional theory (DFT) calculations. The lowest-lying excited state of Ru-bpm is described as a (Ru → bpm) metal-to-ligand charge-transfer (MLCT) state, while the metal-centered (MC) excited state was found computationally to be close in energy to the lowest-energy bright MLCT state (MC state was 0.16 eV above the MLCT state). The excited-state kinetics of Ru-bpm were found via transient absorption spectroscopy to be short-lived and were fit well to a biexponential function with lifetimes $τ_1$ = 4 ps and $τ_2$ = 65 ps in aqueous solution. Kinetic isotope effects of 1.75 ($τ_1$) and 1.61 ($τ_2$) were observed for both decay components, indicating that the solvent plays an important role in the excited-state dynamics of Ru-bpm. Based on the pH-dependent studies and the results from prior studies of similar Ru-complexes, we hypothesize that the 3 MLCT state forms an excited-state hydrogen-bond adduct with the solvent molecules and that this process occurs with a 4 ps lifetime. The formation of such a hydrogen-bond complex is consistent with the electronic density accumulation at the peripheral N atoms of the bpm moiety in the 3 MLCT state. The hydrogen-bonded state 3 MLCT decays to the ground state with a 65 ps lifetime. Such a short lifetime is likely associated with the efficient vibrational energy transfer from the 3 MLCT state to the solvent.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Coupled Roles of Surface Chemistry and Hydrogen-Assisted Cycling in Ruthenium Atomic Layer Deposition on Silicon Oxides

Ruthenium (Ru) is a promising interconnect material for advanced semiconductor technologies due to its favorable scaling characteristics, including a short electron mean free path and strong electromigration resistance. In semiconductor integration, silicon oxide-based dielectrics serve as dominant insulating materials and constitute ubiquitous interfaces for metallization; however, their formation-dependent surface chemistry and its impact on Ru growth remain insufficiently explored. Here, we investigate Ru ALD on native oxide SiO x (N-SiO x ) and thermally grown SiO 2 (T-SiO 2 ) as model substrates using bis(ethylcyclopentadienyl)ruthenium(II) [Ru(EtCp) 2 ] under two distinct reactant-sequence environments: AB-type (Ru(EtCp) 2 /O 2 ) and hydrogenassisted ABC-type (Ru(EtCp) 2 /O 2 /H 2 ). Under the AB-type process, both N-SiO x and T-SiO 2 exhibit pronounced nucleation delay. N-SiO x shows earlier nucleation and higher nucleation density than T-SiO 2 , plausibly attributed to differences in surface hydroxyl populations. Similar temperature-dependent phase evolution is observed on both substrates, with mixed Ru and RuO 2 phases at 250 °C and predominantly metallic Ru at 300 °C accompanied by increased morphological roughening. In contrast, incorporating an H 2 subpulse (ABC-type) mitigates nucleation delay, particularly on hydroxyl-deficient T-SiO 2 , thereby reducing the substratedependent disparity observed under AB cycling. Moreover, RuO 2 formation is suppressed even at 250 °C on both substrates, shifting growth toward more metallic Ru with reduced resistivity (∼20 μΩ·cm at ∼ 20 nm on N-SiO x ). These trends suggest that H 2 influences the surface reaction pathway, contributing to enhanced metallic stabilization and altered early stage growth kinetics. Overall, this work clarifies the coupled roles of substrate chemistry and reactant-sequence design in governing Ru nucleation and early stage film evolution, providing insight relevant to next-generation interconnect integration and future area-selective deposition strategies.

36 MATERIALS SCIENCE↗

Deciphering the Mechanism of Base-Triggered Conversion of Ammonia to Molecular Nitrogen and Methylamine to Cyanide

Here we report an in-depth investigation into the ammonia oxidation mechanism by the catalyst [Ru III (tpy)(dmabpy)NH 3 ] 3 + ([Ru(NH 3 )] 3 + ). Stoichiometric reactions of [Ru(NH 3 )] 3 + were carried out with exogenous noncoordinating bases to trigger a proposed redox disproportionation reaction, which was followed using variable-temperature NMR spectroscopy. An intermediate species was identified as a dinitrogen-bridged complex using 15 N NMR and Raman spectroscopy on isotopically labeled complexes. This intermediate is proposed to derive from coupling of nitridyl species formed upon sequential redox disproportion reactions. Acetonitrile displaces the dinitrogen bridge to yield free N 2 . DFT calculations support this lower-energy pathway versus that previously reported for ammonia oxidation by the parent [Ru III (tpy)(bpy)NH 3 ] 3 + complex. These experimental and computational results are consistent with the interpretation of redox disproportionation involving sequential hydrogen atom transfer reactions by an amide/aminyl intermediate, [Ru(NH 2 ) – ] + $\Leftrightarrow$ [Ru(NH 2 ) • ] + , formed upon deprotonation of the parent complex. Control experiments employing a large excess of ammonia as a base indicate this new proposed lower-energy pathway contributes to the oxidation of ammonia to dinitrogen in conditions relevant to electrocatalysis. In addition, analogous methylamine complexes, [Ru(NH 2 CH 3 )] 2 + /3 + , were prepared to further test the proposed mechanism. Treating [Ru(NH 2 CH 3 )] 3 + with a base cleanly yields two products [Ru(NH 2 CH 3 )] 2 + and [Ru(CN)] + in an ~3:1 ratio, fully consistent with the proposed cascade of hydrogen atom transfer reactions by an intermediate.

37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CH↗

Fundamental Studies of Bifunctional Catalysts for Tandem Reactions

During the past few years of our funding from DOE Basic Energy Sciences, we have focused on the catalytic conversion of biomass-derived 5-hydroxymethyl furfural (HMF) as a platform molecule for sustainable synthesis of value-added chemicals. The combination of the diene and aldehyde functionalities in HMF enables catalytic production of acetalized HMF derivatives with diol or epoxy reactants to allow reversible synthesis of norcantharimide derivatives upon Diels-Alder reaction with maleimides. Whereas the electron-withdrawing nature of aldehyde group inhibits the reactivity of diene group in HMF to undergo Diels-Alder reactions with dienophiles, by converting the aldehyde group in HMF to an electron-donating hydroxyl group, HMF can append maleimide-based chemicals through Diels-Alder coupling. Acetalization of HMF not only produces an electron-rich diene for Diels-Alder reaction, but it also alters the reversibility of acetal formation and thereby allows for the controlled release of chemicals by hydrolysis. Therefore, we synthesized various norcantharimide derivatives from biomass-derived HMF by acetalization over an acid catalyst, Amberlyst-15, followed by Diels-Alder reaction with maleimide. The norcantharimides release the starting materials by retro Diels-Alder reaction that is triggered by acetal hydrolysis under acidic (≤pH 3) conditions. In subsequent work, we explored the synthesis and properties of functional polyurethanes and polyesters with tunable properties from biomass-derived (HMF)-Acetone-HMF (HAH) monomers. HAH can be selectively hydrogenated over Cu and Ru catalysts to produce partially-hydrogenated HAH (PHAH) and fully-hydrogenated HAH (FHAH). HAH contains functional groups, including hydroxyl, furan, enone, and ketone functionalities, that can be exploited to further tune the polymer properties. The π-electron conjugation between the enone and furan groups in HAH monomer stabilizes the furan group to prevent the uncontrolled degradation of furans during reactions, such as etherification. Therefore, HAH is a renewable monomer that can be used to synthesize polymers, having high molecular weight, symmetric functionalities, an inexpensive production price, and being derived from renewable resources without competition with food resources. We demonstrated the synthesis of functional polyurethanes and a renewable polyester from HAH-derived monomers, and 4,4’-methylenebis(phenyl isocyanate) (MDI). We showed that it is essential to be able to selective hydrogenate C=C double bonds in HAH to be able to achieve effective Diels Alder reactions of the furan ring. Therefore, we studied the hydrogenation at temperatures from 313 – 393 K of HAH over Pd, Ru, and Cu based catalysts. HAH was selectively hydrogenated to produce partially-hydrogenated monomers (PHAH) over Cu and Ru catalysts and to fully-hydrogenated HAH monomers (FHAH) over the Ru catalyst. Pd based catalysts yielded a mixture of partially and fully hydrogenated monomers. Reaction kinetics models were employed to quantify the kinetic behavior for hydrogenation over Ru, Cu, and Pd catalysts. A 5-step pathway exhibited over Pd and Ru catalysts consists of both series and parallel reaction steps, where HAH is both converted to fully hydrogenated products sequentially via series reactions of partially hydrogenated intermediates, as well as converted directly in parallel reactions to form the fully hydrogenated products. In contrast, a 3-step pathway over the Cu catalyst consists only of the consecutive reaction steps, where the final product was formed via series reactions of intermediate products. Additionally, reaction over the Cu catalyst did not hydrogenate the furan rings of the HAH molecule and yielded a different final product than those hydrogenation over Pd and Ru catalysts. Using the results from our detailed reaction kinetics studies, we developed universal conditions for the maximum production of the various hydrogenated products for both batch and plug flow systems. In subsequent work, we employed reaction schemes to optimize the yields of products from selective hydrogenations of HAH in isopropanol solvent and in the presence of liquid water. Reaction schemes consisting of 7, 9, and 11 steps were examined to describe the rates of formation of the observed products and reaction intermediates for hydrogenation of HAH over Ru and Pd catalysts, and a 3-step scheme was studied over Cu catalysts. Rate constants and activation energies were calculated using these reaction schemes, and we then apply these reaction schemes to explore the effects of water addition on the hydrogenation pathways. The effects of water addition to isopropanol (IPA) solvents on the hydrogenation of HAH were markedly different over Pd, Ru, and Cu catalysts. Over the Pd catalyst, the addition of water to IPA increased hydrogenation rates and promoted hydrogenation of furan rings. The addition of water to IPA yielded significant carbon losses over the Ru catalyst, and slowed hydrogenation steps over Cu, while significantly inhibiting hydrogenation of the ketone group. This behavior opened routes toward increased production rates of PHAH=O (a partially hydrogenated form of HAH containing a C=O bond), a product in which the diene groups of the furan rings were not hydrogenated. Addition of water also allowed increased feed concentrations of HAH that were previously not possible in pure IPA solvents.

09 BIOMASS FUELS↗

Developing a Fundamental Knowledge Base for the Interaction of Ruthenium with Natural and Engineered Iron-Bearing Materials

The intent of this project is to build a fundamental knowledge base concerning the redox coupling between Ru and Fe in heterogeneous systems with predictive applications towards the fate, speciation, and transport of Ru in the environment and its capture using available technologies. RuNOCl 3 and Fe 3+ are redox active over a broad range of pH. Initial assessment of effect of redox coupling between Ru and Fe indicates that Fe(III) in ferrihydrite can oxidize Ru 2+ in RuNOCl3 to Ru(IV) during coprecipitation at ambient conditions and alkaline pH. Further, evidence suggests that Ru(IV) is incorporated in the structure of fh. Likewise, Fe 3+ (aq) also reduces Ru 2+ in RuNOCl 3 in the homogenous system at acidic pH although the kinetics of reaction appear to be slow. Rufh annealed to 500 0C transforms to Ru(III) doped hematite. AIMD informed EXAFS indicates that Ru substitutes for Fe(III) in regular octahedral sites of hematite but requires three distinct configurations involving edge-sharing protonated Fe vacancies and straight substitution with no local defects. Fe 2+ (aq) appears to oxidize at the surface of RuO 2 , but the amount is too low to reasonably expect detectable reduced Ru. Future experiments at higher pH are warranted to make Fe 2+ (aq) less stable (i.e., make more redox active). We also demonstrated that we can functionalize Si aerogels with Fe(II) and Fe(III) but likely need to go to higher T to make Feo nanoparticles.

36 MATERIALS SCIENCE↗

Materials Data on TiPRu by Materials Project

TiRuP crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Ti is bonded in a 11-coordinate geometry to six equivalent Ru and five P atoms. There are two shorter (2.78 Å) and four longer (2.92 Å) Ti–Ru bond lengths. There are one shorter (2.61 Å) and four longer (2.63 Å) Ti–P bond lengths. Ru is bonded in a 12-coordinate geometry to six equivalent Ti, two equivalent Ru, and four P atoms. Both Ru–Ru bond lengths are 2.72 Å. There are two shorter (2.39 Å) and two longer (2.42 Å) Ru–P bond lengths. There are two inequivalent P sites. In the first P site, P is bonded in a 9-coordinate geometry to three equivalent Ti and six equivalent Ru atoms. In the second P site, P is bonded in a 9-coordinate geometry to six equivalent Ti and three equivalent Ru atoms.

36 MATERIALS SCIENCE↗

Materials Data on HfPRu by Materials Project

HfRuP crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Hf is bonded in a 11-coordinate geometry to six equivalent Ru and five P atoms. There are two shorter (2.88 Å) and four longer (3.01 Å) Hf–Ru bond lengths. There are one shorter (2.68 Å) and four longer (2.71 Å) Hf–P bond lengths. Ru is bonded to six equivalent Hf, two equivalent Ru, and four P atoms to form a mixture of distorted corner, edge, and face-sharing RuHf6P4Ru2 cuboctahedra. Both Ru–Ru bond lengths are 2.75 Å. All Ru–P bond lengths are 2.47 Å. There are two inequivalent P sites. In the first P site, P is bonded in a 9-coordinate geometry to six equivalent Hf and three equivalent Ru atoms. In the second P site, P is bonded in a 9-coordinate geometry to three equivalent Hf and six equivalent Ru atoms.

36 MATERIALS SCIENCE↗

Materials Data on ScPRu by Materials Project

ScRuP crystallizes in the hexagonal P-62m space group. The structure is three-dimensional. Sc is bonded in a 11-coordinate geometry to six equivalent Ru and five P atoms. There are two shorter (2.91 Å) and four longer (2.97 Å) Sc–Ru bond lengths. There are four shorter (2.69 Å) and one longer (2.70 Å) Sc–P bond lengths. Ru is bonded in a 12-coordinate geometry to six equivalent Sc, two equivalent Ru, and four P atoms. Both Ru–Ru bond lengths are 2.78 Å. There are two shorter (2.43 Å) and two longer (2.53 Å) Ru–P bond lengths. There are two inequivalent P sites. In the first P site, P is bonded in a 9-coordinate geometry to six equivalent Sc and three equivalent Ru atoms. In the second P site, P is bonded in a 9-coordinate geometry to three equivalent Sc and six equivalent Ru atoms.

36 MATERIALS SCIENCE↗