2020
DOI: 10.1038/s41427-020-0210-2
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Relationship between magnetic nucleation and the microstructure of a hot-deformed permanent magnet: micromagnetic simulation

Abstract: The grains initiating magnetization reversal in the microstructure of a hot-deformed permanent magnet have been identified in this study by performing micromagnetic simulations based on the Landau-Lifshitz-Gilbert equation. Hotdeformed permanent magnets comprise tabular grains, the easy-axis orientations of which are inclined with respect to the nominal easy axis of the permanent magnet. In the simulation model, the grains complexly overlap, similar to in actual permanent magnets. We analyze the simulation res… Show more

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Cited by 8 publications
(6 citation statements)
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“…In figure 2(b) almost the same behaviors are observed as before, except that the magnetization near the compensation point is badly figured because of the appearance of some fluctuations, and this could be due to the weak J int J sh , which equals −0.1 in this case, so the correlation is much weaker between the core and shell spins [34]. One could also assume that spin canting occurs at the interface, where reduced interfacial exchange interaction allows spins closest to the interface to deviate locally from collinear structures [35].…”
Section: J Stat Mech (2023) 033209supporting
confidence: 73%
See 1 more Smart Citation
“…In figure 2(b) almost the same behaviors are observed as before, except that the magnetization near the compensation point is badly figured because of the appearance of some fluctuations, and this could be due to the weak J int J sh , which equals −0.1 in this case, so the correlation is much weaker between the core and shell spins [34]. One could also assume that spin canting occurs at the interface, where reduced interfacial exchange interaction allows spins closest to the interface to deviate locally from collinear structures [35].…”
Section: J Stat Mech (2023) 033209supporting
confidence: 73%
“…Cubic anisotropy is generally much weaker than uniaxial anisotropy, and has three principal directions which energetically are easy, hard and very hard magnetization directions respectively [28]. It is worth noting that in the case of low anisotropy, each particle constituting the system rotates coherently [28], however, for high anisotropy it is energetically favorable for the system to form domain walls [33,34]. Finally, the last term in equation ( 1) accounts for the interaction of the system spins with the applied external magnetic field B.…”
Section: Computational Detailsmentioning
confidence: 99%
“…The macroscopic properties of permanent magnets arise from the interplay of intrinsic material properties and the magnet's granular microstructure. Traditionally, structural characterization [1], imaging and magnetic measurements [2,3] as well as micromagnetic theory [4] and simulations [5][6][7] have been applied to obtain a better understanding of the impact of microstructure on the magnetic properties. The relation between structure and properties can be treated as mapping between an input space and an ouput space.…”
Section: Introductionmentioning
confidence: 99%
“…The laborious optimization of Nd-Fe-B magnets toward the desired microstructure and magnetic performance is still in progress [9][10][11][12][13][14][15][16] . To accelerate this process, micromagnetic simulations are often used to elucidate the relationship between the microstructural features and macroscopic magnetic properties 6,[17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] . Current micromagnetic models of Nd-Fe-B magnets address two cases of high practical importance: sintered magnets 6,8,[20][21][22][23] and hot-deformed ones [24][25][26][27][28][29][30][31][32][33] .…”
mentioning
confidence: 99%