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Materials Data on Sm2O3 by Materials Project

Sm2O3 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. Sm3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Sm–O bond distances ranging from 2.28–2.66 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Sm3+ atoms to form OSm4 tetrahedra that share corners with six equivalent OSm6 octahedra, corners with six equivalent OSm4 tetrahedra, edges with three equivalent OSm6 octahedra, and edges with three equivalent OSm4 tetrahedra. The corner-sharing octahedra tilt angles range from 18–56°. In the second O2- site, O2- is bonded to six equivalent Sm3+ atoms to form OSm6 octahedra that share corners with twelve equivalent OSm4 tetrahedra, edges with six equivalent OSm6 octahedra, and edges with six equivalent OSm4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Sm2O3 by Materials Project

Sm2O3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Sm3+ sites. In the first Sm3+ site, Sm3+ is bonded to six O2- atoms to form a mixture of distorted edge and corner-sharing SmO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Sm–O bond distances ranging from 2.28–2.57 Å. In the second Sm3+ site, Sm3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Sm–O bond distances ranging from 2.31–2.81 Å. In the third Sm3+ site, Sm3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Sm–O bond distances ranging from 2.31–2.69 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded to six Sm3+ atoms to form OSm6 octahedra that share corners with six OSm4 tetrahedra, corners with two equivalent OSm4 trigonal pyramids, edges with two equivalent OSm6 octahedra, edges with four equivalent OSm5 square pyramids, and edges with six OSm4 tetrahedra. In the second O2- site, O2- is bonded to four Sm3+ atoms to form OSm4 tetrahedra that share corners with two equivalent OSm6 octahedra, corners with two equivalent OSm5 square pyramids, corners with four OSm4 tetrahedra, corners with six equivalent OSm4 trigonal pyramids, an edgeedge with one OSm6 octahedra, edges with two equivalent OSm5 square pyramids, and an edgeedge with one OSm4 tetrahedra. The corner-sharing octahedral tilt angles are 14°. In the third O2- site, O2- is bonded to four Sm3+ atoms to form distorted OSm4 trigonal pyramids that share a cornercorner with one OSm6 octahedra, corners with two equivalent OSm5 square pyramids, corners with nine OSm4 tetrahedra, corners with two equivalent OSm4 trigonal pyramids, edges with three equivalent OSm5 square pyramids, and edges with two equivalent OSm4 trigonal pyramids. The corner-sharing octahedral tilt angles are 36°. In the fourth O2- site, O2- is bonded to four Sm3+ atoms to form OSm4 tetrahedra that share a cornercorner with one OSm6 octahedra, corners with five equivalent OSm5 square pyramids, corners with four OSm4 tetrahedra, corners with three equivalent OSm4 trigonal pyramids, edges with two equivalent OSm6 octahedra, an edgeedge with one OSm5 square pyramid, and edges with two equivalent OSm4 tetrahedra. The corner-sharing octahedral tilt angles are 50°. In the fifth O2- site, O2- is bonded to five Sm3+ atoms to form distorted OSm5 square pyramids that share corners with seven OSm4 tetrahedra, corners with two equivalent OSm4 trigonal pyramids, edges with two equivalent OSm6 octahedra, edges with two equivalent OSm5 square pyramids, edges with three OSm4 tetrahedra, and edges with three equivalent OSm4 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Sm2O3 by Materials Project

Sm2O3 is Corundum-like structured and crystallizes in the cubic Ia-3 space group. The structure is three-dimensional. there are two inequivalent Sm3+ sites. In the first Sm3+ site, Sm3+ is bonded to six equivalent O2- atoms to form a mixture of distorted edge and corner-sharing SmO6 octahedra. The corner-sharing octahedral tilt angles are 57°. All Sm–O bond lengths are 2.37 Å. In the second Sm3+ site, Sm3+ is bonded to six equivalent O2- atoms to form a mixture of distorted edge and corner-sharing SmO6 octahedra. The corner-sharing octahedra tilt angles range from 55–57°. There are four shorter (2.34 Å) and two longer (2.43 Å) Sm–O bond lengths. O2- is bonded to four Sm3+ atoms to form a mixture of distorted edge and corner-sharing OSm4 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Sm2O3 by Materials Project

Sm2O3 crystallizes in the cubic Pn-3m space group. The structure is three-dimensional. Sm3+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms. All Sm–O bond lengths are 2.36 Å. O2- is bonded to four equivalent Sm3+ atoms to form a mixture of corner and edge-sharing OSm4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Sm2O3 by Materials Project

Sm2O3 crystallizes in the tetragonal P-4m2 space group. The structure is three-dimensional. Sm3+ is bonded in a 6-coordinate geometry to six O2- atoms. There are four shorter (2.30 Å) and two longer (2.54 Å) Sm–O bond lengths. There are three inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Sm3+ atoms to form a mixture of edge and corner-sharing OSm4 tetrahedra. In the second O2- site, O2- is bonded to four equivalent Sm3+ atoms to form a mixture of edge and corner-sharing OSm4 tetrahedra. In the third O2- site, O2- is bonded to four equivalent Sm3+ atoms to form a mixture of edge and corner-sharing OSm4 tetrahedra.

36 MATERIALS SCIENCE↗

Effects of processing parameters on the morphologies of complex sesquioxide thin films

Controlling and predicting the morphology of lanthanide sesquioxides in thin film form is vital to their use in current applications. In the present study, single and codeposited Sm2O3, Er2O3, and Lu2O3 thin films were grown on yttria-stabilized zirconia (8%) substrates by radio frequency magnetron sputtering at room temperature and 500 °C. The effect of two different substrate temperatures and altering the oxide cation on the structural and morphological properties of the films was analyzed. The thin films were characterized by profilometry, scanning electron microscopy, transmission electron microscopy, and x-ray diffraction. The single-component Lu2O3 and Sm2O3 films obtained were of the cubic phase, and the Er2O3 was a mix of cubic and monoclinic phases. It was observed for both the Er2O3 and Lu2O3 films that increasing the substrate temperature to 500 °C resulted in larger grained polycrystalline films. In contrast, large grained polycrystalline films were obtained at both room temperature and 500 °C for Sm2O3 and uneven granularity increased as temperature increased. Codeposition of Lu2O3 and Sm2O3, and Lu2O3 and Er2O3 resulted in a cubic bixbyite phase (the C phase of the lanthanide sesquioxide) solid solution. It was observed that the structure and morphology of the films can be controlled by manipulating deposition parameters. Both substrate temperature and altering the oxide cation contributed to changes in crystallinity and grain structure, which can modify the chemical and physical properties of the films for their applications.

36 MATERIALS SCIENCE↗

Effects of additives on volume change on melting, surface tension, and viscosity of liquid aluminum oxide

The effects of various oxide additives on the volume change on melting, the surface tension, and the viscosity of liquid Al2O3 were studied. Additives of Sm2O3, MgO, and Y2O3 which form solid solutions, compounds, and multiphase solids with Al2O3 were studied. A review of the property data for Al2O3 and Al2O3 containing oxide additives is presented. Oxide additives to Al2O3 reduce the volume change on melting and with the exception of SiO2 lower the viscosity; surface tensions change with oxide additives, but changes vary with different container material. Viscosity and volume change on melting appeared to be significantly more important for studying the properties of liquid oxides than surface tension. Supercooling of 270 K of yttrium aluminum garnet was observed.

Bates, J. L.↗

Strength and microstructure of sintered Si3N4 with rare-earth-oxide additions

Room temperature, 700-, 1000-, 1200-, and 1370-C examinations of the effect of 1.7-2.6 mol pct rare earth oxide additions to sintered Si3N4 are conducted. While the room temperature-1000 C bend strengths were higher for this material with Y2O3 additions than with CeO2, La2O3, or Sm2O3, the reverse was true at 1200-1370 C. This phenomenon is explained on the basis of microstructural differences, since quantitative microscopy of SEM replicas showed the Si3N4-Y2O3 composition to contain both a higher percentage of elongated grains and a coarser microstructure than the other three alternatives. The elongated grains appear to increase this composition's low temperature strength irrespective of microstructural coarseness; this coarseness, however, decreases strength relative to the other compositions at higher temperatures.

Sanders, W. A.↗

Oxidation of silicon nitride sintered with rare-earth oxide additions

The effects of rare-earth oxide additions on the oxidation of sintered Si3N4 were examined. Insignificant oxidation occurred at 700 and 1000 C, with no evidence of phase instability. At 1370 C, the oxidation rate was lowest for Y2O3 and increased for additions of La2O3, Sm2O3, and CeO2, in that order. Data obtained from X-ray diffraction, electron microprobe analysis, and scanning electron microscopy indicate that oxidation occurs via diffusion of cationic species from Si3N4 grain boundaries.

Mieskowski, D. M.↗

Thermodynamic properties of some metal oxide-zirconia systems

Metal oxide-zirconia systems are a potential class of materials for use as structural materials at temperatures above 1900 K. These materials must have no destructive phase changes and low vapor pressures. Both alkaline earth oxide (MgO, CaO, SrO, and BaO)-zirconia and some rare earth oxide (Y2O3, Sc2O3, La2O3, CeO2, Sm2O3, Gd2O3, Yb2O3, Dy2O3, Ho2O3, and Er2O3)-zirconia system are examined. For each system, the phase diagram is discussed and the vapor pressure for each vapor species is calculated via a free energy minimization procedure. The available thermodynamic literature on each system is also surveyed. Some of the systems look promising for high temperature structural materials.

Jacobson, Nathan S.↗

Mechanically robust high magnetic-performance Sm-Co sintered magnets through microstructure engineering

Samarium-cobalt (Sm-Co) sintered magnets have high magnetic energy densities, great resistance to demagnetization and corrosion, and excellent thermal stability in a wide temperature range (–50–550 °C). However, the utilization of these magnets is restricted by their brittleness. Based on micromechanical and the Zener pinning model, Sm-Co sintered magnets with improved mechanical properties have been designed and fabricated via microstructure engineering. A small amount of fine Sm 2 O 3 particulates (0–3 wt%) has been incorporated into Sm 2 (CoFeCuZr) 17 sintered magnets to refine the grain size by up to approximately 50% (from 45 to 22 µm) and narrow the grain size distribution. Doping with 3 wt% Sm 2 O 3 increased the flexural strength by 62% while maintaining magnetic performance. Both grain-refined unimodal microstructure and heterogeneous laminated coarse/fine grain microstructure were formed by strategically designed assemblies of Sm 2 O 3 -added Sm-Co powder feedstock mixtures. The technology is compatible with existing magnet manufacturing processes. Numerical micromechanics simulation indicates that the fracture is dominated by intragranular mode. The mechanical strength is mainly enhanced by the additive-induced grain refinement, while the small amount of Sm 2 O 3 addition has a small direct positive contribution. Finally, these magnets will be more cost-effective, efficient, and robust for various functional applications.

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