journal article·2017-05-01Open access

Micromagnetic simulation for the magnetization reversal process of Nd-Fe-B hot-deformed nanocrystalline permanent magnets

Hiroshi Tsukahara, Kaoru Iwano, Chiharu Mitsumata, Tadashi Ishikawa, Kanta Ono

AIP Advances· Volume 7· Issue 5

Abstract

We numerically demonstrated the magnetization reversal process inside a hot-deformed nanocrystalline permanent magnet. We performed large-scale micromagnetics simulation based on the Landau–Lifshitz–Gilbert equation with 0.1 billion calculation cells. The simulation model for the hot-deformed nanocrystalline permanent magnet consists of 2622 tabular grains that interact with each other by inter-grain exchange and dipole interactions. When the strength of the external field approached a coercive force, nucleation cores were created at the grain surface. The magnetization reversal was propagated by the inter-grain and dipole interactions. When the grains had overlapping regions parallel to the external field, the magnetization reversal propagated quickly between the grains due to the dipole interaction. In contrast, the motion of the magnetic domain wall was inhibited at interfaces between the grains perpendicular to the external field. Reversal magnetic domains had a pillar-shaped structure that is parallel to the external field. In the perpendicular direction, the reversal magnetic domain expanded gradually because of the inhibition of the domain wall motion.
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Research context

OpenAlex topics: Magnetic Properties of Alloys · Magnetic properties of thin films · Magnetic Properties and Applications

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

High Energy Accelerator Research Organization (KEK) 1 , Tsukuba 305-0801, Japan

National Institute for Materials Science (NIMS) 2 , Tsukuba 305-0047, Japan

Funding

Japan Science and Technology Agency

References (18)

Show source-provided references
1. Appl. Phys. Lett. · 1984 · 44 · 14810.1063/1.94584 ↗
2. IEEE Trans. Magn. · 1985 · 21 · 195810.1109/tmag.1985.1064031 ↗
3. Apll. Phys. Lett. · 1986 · 48 · 73310.1063/1.96704 ↗
4. Scr. Mater. · 2013 · 69 · 64710.1016/j.scriptamat.2013.07.011 ↗
5. Phys. Rev. B · 1994 · 49 · 610010.1103/physrevb.49.6100 ↗
6. J. Appl. Phys. · 1996 · 79 · 502910.1063/1.361565 ↗
7. J. Magn. Magn. Mater · 1997 · 171 · 6910.1016/s0304-8853(97)00066-8 ↗
8. Scr. Mater. · 2013 · 61 · 6622
9. Scr. Mater. · 2013 · 68 · 16710.1016/j.scriptamat.2012.10.005 ↗
10. Acta Mater. · 2013 · 61 · 538710.1016/j.actamat.2013.05.027 ↗
11. IEEE Trans. Magn. · 2014 · 50 · 710070410.1109/tmag.2014.2326176 ↗
12. IEEE Trans. Magn. · 2015 · 51 · 710010410.1109/tmag.2015.2436411 ↗
13. IEEE. Trans. Magn. · 2014 · 50 · 140030410.1109/tmag.2013.2278221 ↗
14. AIP Advance · 2016 · 6 · 05640510.1063/1.4944338 ↗
15. Comput. Phys. Commun. · 2016 · 207 · 21710.1016/j.cpc.2016.06.013 ↗
16. J. Phys. D: Appl. Phys. · 2000 · 33 · R13510.1088/0022-3727/33/15/201 ↗
17. Appl. Phys. Lett. · 1999 · 74 · 174910.1063/1.123676 ↗
18. J. Appl. Phys. · 2012 · 111 · 10390110.1063/1.4712635 ↗