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Materials Data on Ce2Fe14B by Materials Project

Ce2Fe14B is beta Uranium-derived structured and crystallizes in the tetragonal P4_2/mnm space group. The structure is three-dimensional. there are two inequivalent Ce sites. In the first Ce site, Ce is bonded in a 3-coordinate geometry to sixteen Fe and one B atom. There are a spread of Ce–Fe bond distances ranging from 3.04–3.36 Å. The Ce–B bond length is 2.90 Å. In the second Ce site, Ce is bonded in a 10-coordinate geometry to sixteen Fe and two equivalent B atoms. There are a spread of Ce–Fe bond distances ranging from 3.00–3.21 Å. Both Ce–B bond lengths are 3.24 Å. There are six inequivalent Fe sites. In the first Fe site, Fe is bonded to two Ce and ten Fe atoms to form a mixture of distorted face, edge, and corner-sharing FeCe2Fe10 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.37–2.65 Å. In the second Fe site, Fe is bonded in a 2-coordinate geometry to two Ce and twelve Fe atoms. There are a spread of Fe–Fe bond distances ranging from 2.64–2.77 Å. In the third Fe site, Fe is bonded to three Ce and nine Fe atoms to form a mixture of distorted face, edge, and corner-sharing FeCe3Fe9 cuboctahedra. There are a spread of Fe–Fe bond distances ranging from 2.42–2.59 Å. In the fourth Fe site, Fe is bonded in a distorted single-bond geometry to two Ce, seven Fe, and one B atom. The Fe–Fe bond length is 2.54 Å. The Fe–B bond length is 2.08 Å. In the fifth Fe site, Fe is bonded in a distorted L-shaped geometry to two equivalent Ce, four Fe, and two equivalent B atoms. Both Fe–B bond lengths are 2.05 Å. In the sixth Fe site, Fe is bonded to four Ce and eight Fe atoms to form a mixture of face and corner-sharing FeCe4Fe8 cuboctahedra. B is bonded in a 6-coordinate geometry to three Ce and six Fe atoms.

36 MATERIALS SCIENCE↗

Magnetic Materials Research at SRNL

Fig: Rietveld Refinement of room temperature PXRD data for annealed Ce2Fe14B (left panel), (Y0.1Ce1.9)Fe14B (middle panel), and (Lu0.1Ce1.90)Fe14B (right panel) alloys. All annealed alloys plotted are composed primarily of Ce2Fe14B phase with small α-Fe impurities. Vertical blue ticks correspond to the position of the calculated Bragg peaks of all phases (from top to bottom, 2-14-1 and α-Fe). Fig: (Left Panel) Field dependent magnetization measurements on aligned powder with the magnetic field applied along the easy direction for annealed Ce2Fe14B and (YxCe2-x)Fe14B (x=0.1, 0.2, 0.3, 0.4, 0.5) alloys. (Middle Panel) Field dependent magnetization measurements on aligned powder with the magnetic field applied along the hard direction for annealed Ce2Fe14B and (YxCe2-x)Fe14B (x=0.1, 0.2, 0.3, 0.4, 0.5) alloys. (Right Panel) The saturation magnetization of Ce2Fe14B and (YxCe2-x)Fe14B (x=0.1, 0.2, 0.3, 0.4, 0.5) alloys as determined from easy axis field dependent magnetization measurements.

Bretana, Alex↗

Magnetic Materials Research at SRNL

Introduction – What are Magnetic Materials? Magnetic materials are crystalline solids which below a certain temperature, known as the ordering temperature, display spontaneous order in their magnetic moments. Results • Enhanced thermal stability and saturation magnetization with Y substitution in Ce2Fe14B based permanent magnets • Discovered a new ferromagnetic phase transition at TC = 62.9 K in (Dy1/3Mo2/3)2AlC and validated the two previously reported low temperature magnetic phases Characterization of Magnetic Materials Raw high purity materials are melted together to synthesize a crystalline sample using an arc melter at Savannah River National Laboratory (SRNL). Use high energy ball milling to form a hard/soft magnetic composite using Y substituted Ce2Fe14B. Finish structural characterization on γ- irradiated (RE1/3Mo2/3)2AlC (RE = Rare Earth) MAX samples. Unit Cell Lattice Points

Bretana, Alex↗