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Materials Data on Dy2O3 by Materials Project

Dy2O3 crystallizes in the trigonal P-3m1 space group. The structure is three-dimensional. Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.21–2.58 Å. There are two inequivalent O2- sites. In the first O2- site, O2- is bonded to four equivalent Dy3+ atoms to form ODy4 tetrahedra that share corners with six equivalent ODy6 octahedra, corners with six equivalent ODy4 tetrahedra, edges with three equivalent ODy6 octahedra, and edges with three equivalent ODy4 tetrahedra. The corner-sharing octahedra tilt angles range from 19–55°. In the second O2- site, O2- is bonded to six equivalent Dy3+ atoms to form ODy6 octahedra that share corners with twelve equivalent ODy4 tetrahedra, edges with six equivalent ODy6 octahedra, and edges with six equivalent ODy4 tetrahedra.

36 MATERIALS SCIENCE↗

Materials Data on Dy2O3 by Materials Project

Dy2O3 is Corundum-like structured and crystallizes in the cubic Ia-3 space group. The structure is three-dimensional. there are two inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded to six equivalent O2- atoms to form a mixture of distorted edge and corner-sharing DyO6 octahedra. The corner-sharing octahedra tilt angles range from 54–56°. There are a spread of Dy–O bond distances ranging from 2.26–2.35 Å. In the second Dy3+ site, Dy3+ is bonded to six equivalent O2- atoms to form a mixture of edge and corner-sharing DyO6 octahedra. The corner-sharing octahedral tilt angles are 56°. All Dy–O bond lengths are 2.30 Å. O2- is bonded to four Dy3+ atoms to form a mixture of distorted edge and corner-sharing ODy4 trigonal pyramids.

36 MATERIALS SCIENCE↗

Materials Data on Dy2O3 by Materials Project

Dy2O3 crystallizes in the monoclinic C2/m space group. The structure is three-dimensional. there are three inequivalent Dy3+ sites. In the first Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.24–2.60 Å. In the second Dy3+ site, Dy3+ is bonded in a 7-coordinate geometry to seven O2- atoms. There are a spread of Dy–O bond distances ranging from 2.24–2.75 Å. In the third Dy3+ site, Dy3+ is bonded to six O2- atoms to form a mixture of edge and corner-sharing DyO6 octahedra. The corner-sharing octahedral tilt angles are 0°. There are a spread of Dy–O bond distances ranging from 2.21–2.48 Å. There are five inequivalent O2- sites. In the first O2- site, O2- is bonded to five Dy3+ atoms to form distorted ODy5 square pyramids that share corners with seven ODy4 tetrahedra, corners with two equivalent ODy4 trigonal pyramids, edges with two equivalent ODy6 octahedra, edges with two equivalent ODy5 square pyramids, edges with three ODy4 tetrahedra, and edges with three equivalent ODy4 trigonal pyramids. In the second O2- site, O2- is bonded to four Dy3+ atoms to form distorted ODy4 trigonal pyramids that share a cornercorner with one ODy6 octahedra, corners with two equivalent ODy5 square pyramids, corners with nine ODy4 tetrahedra, corners with two equivalent ODy4 trigonal pyramids, edges with three equivalent ODy5 square pyramids, and edges with two equivalent ODy4 trigonal pyramids. The corner-sharing octahedral tilt angles are 37°. In the third O2- site, O2- is bonded to six Dy3+ atoms to form ODy6 octahedra that share corners with six ODy4 tetrahedra, corners with two equivalent ODy4 trigonal pyramids, edges with two equivalent ODy6 octahedra, edges with four equivalent ODy5 square pyramids, and edges with six ODy4 tetrahedra. In the fourth O2- site, O2- is bonded to four Dy3+ atoms to form ODy4 tetrahedra that share corners with two equivalent ODy6 octahedra, corners with two equivalent ODy5 square pyramids, corners with four ODy4 tetrahedra, corners with six equivalent ODy4 trigonal pyramids, an edgeedge with one ODy6 octahedra, edges with two equivalent ODy5 square pyramids, and an edgeedge with one ODy4 tetrahedra. The corner-sharing octahedral tilt angles are 13°. In the fifth O2- site, O2- is bonded to four Dy3+ atoms to form ODy4 tetrahedra that share a cornercorner with one ODy6 octahedra, corners with five equivalent ODy5 square pyramids, corners with four ODy4 tetrahedra, corners with three equivalent ODy4 trigonal pyramids, edges with two equivalent ODy6 octahedra, an edgeedge with one ODy5 square pyramid, and edges with two equivalent ODy4 tetrahedra. The corner-sharing octahedral tilt angles are 49°.

36 MATERIALS SCIENCE↗

Materials Data on Dy2O3 by Materials Project

Dy2O3 crystallizes in the cubic Pn-3m space group. The structure is three-dimensional. Dy3+ is bonded in a 6-coordinate geometry to six equivalent O2- atoms. All Dy–O bond lengths are 1.95 Å. O2- is bonded to four equivalent Dy3+ atoms to form a mixture of edge and corner-sharing ODy4 tetrahedra.

36 MATERIALS SCIENCE↗

Mechanism of enhanced critical fields and critical current densities of MgB2 wires with C/Dy$^{2}$O3 co-additions

A series of monofilamentary powder-in-tube MgB2 wires were fabricated with 2 mol. % C doping and co-additions of 0–3 wt. % Dy2O3. Irreversibility fields (μ0Hirr), upper critical fields (μ0Hc2), and transport critical currents were measured, and from these quantities, anisotropies (γ) and electronic diffusivities (Dπ,σ) were estimated. The addition of 1 wt. % Dy2O3 to already optimally C-doped MgB2 wires produced higher Hc2//ab, Hc2//c, and Hirr values at 4.2 K. In addition, the critical current density, Jc, increased with Dy2O3 concentration up to 1 wt. % where non-barrier Jc reached 4.35 × 104 A/cm2 at 4.2 K, 10 T. At higher temperatures, for example, 20 K and 5 T, co-additions of 2 mol. % C and 2 wt. % Dy2O3 improved non-barrier Jc by 40% and 93% compared to 2 and 3 mol. % C doping, respectively. On the other hand, measurements of Tc showed that C/Dy2O3 co-additions increase interband scattering rates at a lower rate than C doping does (assuming C doping levels giving similar levels of low-T μ0Hc2 increase as co-addition). Comparisons to a two-band model for μ0Hc2 in MgB2 allowed us to conclude that the increases in Hc2//ab, Hc2//c, and Hirr (as well as concomitant increases in high-field Jc) with Dy2O3 addition are consistent with increases primarily in intraband scattering. This suggests C/Dy2O3 co-addition to be a more promising candidate for improving non-barrier Jc of MgB2 at temperatures above 20 K.

36 MATERIALS SCIENCE↗