Weak Ferromagnetism in NiS 2 under Nanocrystallization

Structurally well-ordered NiS 2 nanocrystals with an average diameter of 27.0 ± 6.5 nm retain the bulk-like two-step antiferromagnetic transitions, as shown by magnetization and heat-capacity measurements. Below the lower transition, the nanocrystals exhibit a hysteretic ferromagnetic response with large coercivity, exchange bias, and a vertical loop shift after field cooling, whereas the M–H response just above the transition is nearly linear. Taken together, these features are best explained by uncompensated surface moments generated where the low-temperature antiferromagnetic order terminates at the nanocrystal surface. The absence of a clear additional bulk-like weak-ferromagnetic component constrains homogeneous-canting models and indirectly favors a domain-wall scenario for the weak ferromagnetism of bulk NiS 2 .

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Publication Details

Journal
Journal of the Physical Society of Japan
Published
2026-09-12
DOI
https://doi.org/10.7566/jpsj.95.103702
Primary Topic
Magnetic and transport properties of perovskites and related materials
Type
article
Field-Weighted Citation Impact
0.00

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article

Weak Ferromagnetism in NiS 2 under Nanocrystallization

Tetsuya Kida, Hayato Miyazaki, Tatsuya Kawae, Hirofumi Ishii et al.
Journal of the Physical Society of Japan
Magnetic and transport properties of perovskites and related materials
article

Weak Ferromagnetism in NiS 2 under Nanocrystallization

Tetsuya Kida, Hayato Miyazaki, Tatsuya Kawae, Hirofumi Ishii, Yoichi Ishiwata, Masashi Nantoh, Tomohiko Yoshinaga, Ojiro Miyazaki, Koichi Kindo, Akira Matsuo
article en

Abstract

Structurally well-ordered NiS 2 nanocrystals with an average diameter of 27.0 ± 6.5 nm retain the bulk-like two-step antiferromagnetic transitions, as shown by magnetization and heat-capacity measurements. Below the lower transition, the nanocrystals exhibit a hysteretic ferromagnetic response with large coercivity, exchange bias, and a vertical loop shift after field cooling, whereas the M–H response just above the transition is nearly linear. Taken together, these features are best explained by uncompensated surface moments generated where the low-temperature antiferromagnetic order terminates at the nanocrystal surface. The absence of a clear additional bulk-like weak-ferromagnetic component constrains homogeneous-canting models and indirectly favors a domain-wall scenario for the weak ferromagnetism of bulk NiS 2 .

Journal of the Physical Society of JapanVol. 95(10)
Kyushu University (JP), Saga University (JP), National Synchrotron Radiation Research Center (TW), RIKEN (JP), RIKEN Nishina Center (JP), The University of Tokyo (JP), Kumamoto University (JP)
Kumamoto University, Japan Society for the Promotion of Science
Affordable and clean energy
Openalex Percentile: Top 28%
Magnetic and transport properties of perovskites and related materials
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Weak Ferromagnetism in NiS 2 under Nanocrystallization — Tetsuya Kida, Hayato Miyazaki, et al. · Journal of the Physical Society of Japan (2026) | TGRS Research Map | TGRS