4.7 Article

Structural and magnetic properties of hard magnetic system Ce(Co1-xFex)4.4Cu0.6 (0 ≤ x ≤ 0.19)

Journal

JOURNAL OF ALLOYS AND COMPOUNDS
Volume 883, Issue -, Pages -

Publisher

ELSEVIER SCIENCE SA
DOI: 10.1016/j.jallcom.2021.160866

Keywords

Permanent magnet; Coercivity; Energy product; Magnetic domains; Microstructure

Funding

  1. Critical Materials Institute, an Energy Innovation Hub - U.S. Department of Energy, Office of Energy Efficiency, and Renewable Energy, Advanced Manufacturing Office
  2. Iowa State University [DE-AC02-07CH11358]

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Ce(Co1-xFex)(4.4)Cu-0.6 is a composite, hard magnetic system based on the CaCu5-type structure, showing unique magnetic properties and microstructure essential for permanent magnets. Heat treatment can lead to the formation of a nanostructure similar to Sm-Co permanent magnets.
The Ce(Co1-xFex)(4.4)Cu-0.6 (0 <= x <= 0.19) is a composite, hard magnetic system that is based on the CaCu5-type structure (1:5). It shows both, unique magnetic and microstructural features that are essential for permanent magnets, e.g., exceptional squareness of the 2nd. quadrant of the magnetization loops and microstructural features typically needed for pinning. Samples solidified in alumina crucibles are coarse grained and often clearly faceted and readily align in a magnetic field. X-ray, SEM, and TEM analyses show a 1:5-type single-phase material when quenched from high temperature, which, after heat treatment, transforms into a laminar coherent nanostructure through the formation of a dense array of extended intercalated regions. These extended intercalated regions are comprised of segments of the Ce2Ni7-type structure (2:7) which segregate into various closely related precipitates forming a nanostructure similar to the SmCo5 Sm2Co17 composites seen in Sm-Co permanent magnets. Based on TEM and Lorentz microscopy of well-aligned single grain particles, the magnetic domains' reversal mechanism is regulated by anisotropy fluctuations occurring along the easy direction of magnetization and strong exchange interactions between the matrix and defects (e.g.: stacking faults). Lorentz microscopy suggests the domain wall is not physically pinned by the defect, but rather is offset/deflected when it interacts with the defect. The Lorentz and magnetization data suggest that defects cause a bending of the moment away from the c axis inside the grains. (C) 2021 Elsevier B.V. All rights reserved.

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