Abstract

High saturation magnetization and hysteresis-less magnetic responses are desirable for nanoparticles in scientific and technological applications. Rare-earth oxides are potentially promising materials because of their paramagnetism and high magnetic susceptibility in the bulk, but the magnetic properties of their nanoparticles remain incompletely characterized. Here, we present full M–H loops for commercial RE2O3 nanoparticles (RE = Er, Gd, Dy, Ho) with radii from 10–25 nm at room temperature and 4 K. The magnetic responses are consistent with two distinct populations of atoms, one displaying the ideal Re3+ magnetic moment and the other displaying a sub-ideal magnetic moment. If all sub-ideal ions are taken to be on the surface, the data are consistent with ≈2−10 nm surface layers of reduced magnetization. The magnetization of the rare-earth oxide nanoparticles at low temperatures (1.3–1.9 T) exceeds that of the best iron-based nanoparticles, making rare-earth oxides candidates for use in next-generation cryogenic magnetic devices that demand a combination of hysteresis-less response and high magnetization.

Highlights

  • High saturation magnetization and hysteresis-less magnetic responses are desirable for nanoparticles in scientific and technological applications

  • The magnetization of the rare-earth oxide nanoparticles at low temperatures (1.3–1.9 T) exceeds that of the best iron-based nanoparticles, making rare-earth oxides candidates for use in next-generation cryogenic magnetic devices that demand a combination of hysteresis-less response and high magnetization

  • Temperature and field-dependent data collected above TN and up to 7 T were fitted to this two-component model, resulting in excellent agreement [Figs. 2(b) and 2(c)]

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Summary

Introduction

Rare-earth oxides are potentially promising materials because of their paramagnetism and high magnetic susceptibility in the bulk, but the magnetic properties of their nanoparticles remain incompletely characterized. Substantial fractions of each individual particle can belong to distinct subpopulations, with local heterogeneity in the chemical composition, surface sites, anisotropy, or strain influencing global particle properties.[22–25] As a result, we model the nanoparticles as composed of two populations of active species, sub-ideal (s), and ideal (i) ions, with the full response given by a population-weighted sum, M1⁄4N

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