2016
DOI: 10.1103/physrevb.94.104433
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Temperature-dependent exchange stiffness and domain wall width in Co

Abstract: The micromagnetic exchange stiffness is a critical parameter in numerical modeling of magnetization dynamics and reversal processes, yet the current literature reports a wide range of values even for such simple and widely used material as Cobalt.With use of ab-intio estimated Heisenberg parameters we calculate the low temperature micromagnetic exchange stiffness parameters for hexagonal-close-packed (HCP) and face-centred cubic Cobalt without previous and our own. For HCP Co they are slightly different in the… Show more

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Cited by 98 publications
(79 citation statements)
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“…5(d). This is different from the low-temperature power-law scaling behavior of m −0.59 as found in cobalt [60], possibly due to the complicated and intrinsically different crystal structure of Nd 2 Fe 14 B.…”
Section: Domain Wallcontrasting
confidence: 78%
“…5(d). This is different from the low-temperature power-law scaling behavior of m −0.59 as found in cobalt [60], possibly due to the complicated and intrinsically different crystal structure of Nd 2 Fe 14 B.…”
Section: Domain Wallcontrasting
confidence: 78%
“…is therefore a better metric to use to compare samples with different saturation magnetizations. The difference between the exchange length from this study of λ ex = 9.7 nm and the previously reported value of 21 nm 20 could be due to differences in grain structure between the patterned and unpatterned films 44 as well as difficulty in mode assignment, n, in prior work where fewer modes are visible.…”
contrasting
confidence: 83%
“…Under a mean field approximation with homogeneous spin systems, the exponent n is 2 [30,46]. However, under more accurate methods, the exponent takes a value different from 2, for example, FePt: n = 1.76 [30], hcp-Co: n = 1.79 [31]. Thus we estimate n to examine the thermal properties for the Nd 2 Fe 14 B, by fitting A(T ) in Fig.…”
Section: B Exchange Stiffness Constantmentioning
confidence: 99%