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2004
DOI: 10.1016/j.jmmm.2003.12.1007
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Micromagnetic modelling and magnetization processes

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Cited by 23 publications
(19 citation statements)
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“…The easy magnetization direction of SmCo 5 is aligned along the c-direction of the lattice, and the magnetocrystalline anisotropy constant ranges from 1.1-2.0 × 10 8 erg cm -3 (1 erg cm -3 = 0.1 J m -3 ); these values are among the highest known for hard magnetic materials. [7][8][9][10] Furthermore, this alloy exhibits a very high Curie temperature (T c = 1020 K), which makes it superior to other classes of permanent magnetic materials, such as FePt (T c = 750 K) and Nd 2 Fe 14 B (T c = 585 K), for high-temperature applications. [11][12][13][14] However, as with other rare-earth metal materials, metallic SmCo 5 nanoparticles are prone to fast oxidation.…”
mentioning
confidence: 99%
“…The easy magnetization direction of SmCo 5 is aligned along the c-direction of the lattice, and the magnetocrystalline anisotropy constant ranges from 1.1-2.0 × 10 8 erg cm -3 (1 erg cm -3 = 0.1 J m -3 ); these values are among the highest known for hard magnetic materials. [7][8][9][10] Furthermore, this alloy exhibits a very high Curie temperature (T c = 1020 K), which makes it superior to other classes of permanent magnetic materials, such as FePt (T c = 750 K) and Nd 2 Fe 14 B (T c = 585 K), for high-temperature applications. [11][12][13][14] However, as with other rare-earth metal materials, metallic SmCo 5 nanoparticles are prone to fast oxidation.…”
mentioning
confidence: 99%
“…In the three-dimensional (3-D) polycrystalline model, the pinning mechanism is so complicated that the enhanced coercivity is discussed using a one-dimensional (1-D) planer model. 15,16 Scholz et al investigated the potential barrier thickness dependence of the pinning field (H pin ) using 1-D micromagnetic simulations. 17 They demonstrated that H pin increases with increasing barrier thickness and saturates at around the domain wall width.…”
Section: Calculation Results and Discussionmentioning
confidence: 99%
“…the anisotropy field H K (16)(17)(18). In particular, intergranular exchange couplig becomes extremely important in nanocrystalline (spring) magnets, for which the exchange length (basically the length of a domain wall, which for these magnets is a few nanometers) is of the order of the grain size; this yields a more homogeneous magnetization distribution and, consequently, enhances their remanence, but, as a countereffect, it decreases their coercivity (19).…”
Section: Resultsmentioning
confidence: 99%
“…However, different simulation jobs have evidenced that the wall-like structure appearing at it acts as a "nucleation" site for the magnetization reversal, yielding coercivity values in the correct order of magnitude if the boundary exchange is a few tens percent of the bulk value (16)(17)(18). As en example, Figure 9 presents the switching field H S required to reverse the magnetization of a grain with a neighbouring grain with (initially) antiparallel magnetization, for an intergranular coupling of 80% the bulk value and for different values of the exchange-to-anisotropy ratio.…”
Section: Resultsmentioning
confidence: 99%