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Materials Data on Er2O3 by Materials Project

Er2O3 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. Er3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Er–O bond distances ranging from 2.18–2.56 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Er3+ atoms to form OEr4 tetrahedra that share corners with six equivalent OEr6 octahedra, corners with six equivalent OEr4 tetrahedra, edges with three equivalent OEr6 octahedra, and edges with three equivalent OEr4 tetrahedra. The corner-sharing octahedra tilt angles range from 19–55°. In the second O2- site, O2- is bonded to six equivalent Er3+ atoms to form OEr6 octahedra that share corners with twelve equivalent OEr4 tetrahedra, edges with six equivalent OEr6 octahedra, and edges with six equivalent OEr4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Er2O3 by Materials Project

Er2O3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Er3+ sites. In the first Er3+ site, Er3+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing ErO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Er–O bond distances ranging from 2.18–2.45 Å. In the second Er3+ site, Er3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Er–O bond distances ranging from 2.22–2.72 Å. In the third Er3+ site, Er3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Er–O bond distances ranging from 2.22–2.55 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded to four Er3+ atoms to form distorted OEr4 trigonal pyramids that share a cornercorner with one OEr6 octahedra, corners with two equivalent OEr5 square pyramids, corners with nine OEr4 tetrahedra, corners with two equivalent OEr4 trigonal pyramids, edges with three equivalent OEr5 square pyramids, and edges with two equivalent OEr4 trigonal pyramids. The corner-sharing octahedral tilt angles are 37°. In the second O2- site, O2- is bonded to four Er3+ atoms to form distorted OEr4 tetrahedra that share corners with two equivalent OEr6 octahedra, corners with two equivalent OEr5 square pyramids, corners with four OEr4 tetrahedra, corners with six equivalent OEr4 trigonal pyramids, an edgeedge with one OEr6 octahedra, edges with two equivalent OEr5 square pyramids, and an edgeedge with one OEr4 tetrahedra. The corner-sharing octahedral tilt angles are 13°. In the third O2- site, O2- is bonded to four Er3+ atoms to form OEr4 tetrahedra that share a cornercorner with one OEr6 octahedra, corners with five equivalent OEr5 square pyramids, corners with four OEr4 tetrahedra, corners with three equivalent OEr4 trigonal pyramids, edges with two equivalent OEr6 octahedra, an edgeedge with one OEr5 square pyramid, and edges with two equivalent OEr4 tetrahedra. The corner-sharing octahedral tilt angles are 49°. In the fourth O2- site, O2- is bonded to six Er3+ atoms to form OEr6 octahedra that share corners with six OEr4 tetrahedra, corners with two equivalent OEr4 trigonal pyramids, edges with two equivalent OEr6 octahedra, edges with four equivalent OEr5 square pyramids, and edges with six OEr4 tetrahedra. In the fifth O2- site, O2- is bonded to five Er3+ atoms to form distorted OEr5 square pyramids that share corners with seven OEr4 tetrahedra, corners with two equivalent OEr4 trigonal pyramids, edges with two equivalent OEr6 octahedra, edges with two equivalent OEr5 square pyramids, edges with three OEr4 tetrahedra, and edges with three equivalent OEr4 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Er2O3 by Materials Project

Er2O3 is Corundum-like structured and crystallizes in the cubic Ia-3 space group. The structure is three-dimensional. there are two inequivalent Er3+ sites. In the first Er3+ site, Er3+ is bonded to six equivalent O2- atoms to form a mixture of distorted edge and corner-sharing ErO6 octahedra. The corner-sharing octahedra tilt angles range from 54–56°. There are a spread of Er–O bond distances ranging from 2.24–2.32 Å. In the second Er3+ site, Er3+ is bonded to six equivalent O2- atoms to form a mixture of edge and corner-sharing ErO6 octahedra. The corner-sharing octahedral tilt angles are 56°. All Er–O bond lengths are 2.27 Å. O2- is bonded to four Er3+ atoms to form a mixture of distorted edge and corner-sharing OEr4 trigonal pyramids.

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↗

Extending SLUSCHI for Automated Diffusion Calculations

We present an extension of the SLUSCHI package (Solid and Liquid in Ultra Small Coexistence with Hovering Interfaces) to enable automated diffusion calculations from first-principles molecular dynamics. While the original SLUSCHI workflow was designed for melting temperature estimation via solid-liquid coexistence, we adapt its input and output handling to isolate the volume search stage and generate one production trajectory suitable for diffusion analysis. Post-processing tools parse VASP outputs, compute mean-square displacements (MSD), and extract tracer diffusivities using the Einstein relation with robust error estimates through block averaging. Diagnostic plots, including MSD curves, running slopes, and velocity autocorrelations, are produced automatically to help identify diffusive regimes. The method has been validated through representative case studies: self-diffusion in Al-Cu liquid alloys, sublattice melting in Li7La3Zr2O12 and Er2O3, interstitial oxygen transport in bcc and fcc Fe, and oxygen diffusivity in Fe-O liquids with variable Si and Al contents. Viscosity and diffusivity are linked through the Stokes-Einstein relation, with composition dependence assessed via simple linear mixing. This capability broadens SLUSCHI from melting-point predictions to transport property evaluation, enabling high-throughput, fully first-principles datasets of diffusion coefficients and viscosities across metals and oxides.

36 MATERIALS SCIENCE↗