2015
DOI: 10.1038/srep11370
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Resonantly excited precession motion of three-dimensional vortex core in magnetic nanospheres

Abstract: We found resonantly excited precession motions of a three-dimensional vortex core in soft magnetic nanospheres and controllable precession frequency with the sphere diameter 2R, as studied by micromagnetic numerical and analytical calculations. The precession angular frequency for an applied static field HDC is given as ωMV = γeffHDC, where γeff = γ〈mΓ〉 is the effective gyromagnetic ratio in collective vortex dynamics, with the gyromagnetic ratio γ and the average magnetization component 〈mΓ〉 of the ground-sta… Show more

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Cited by 17 publications
(14 citation statements)
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“…As reported in ref. 13 , the value of 〈 m Λ 〉 varies markedly with 2 R in vortex-state spheres (〈 m Λ 〉 = 1 for single-domain spheres). In the present results, it was quite noticeable that the core reversal’s frequency is a function of both 〈 m Λ 〉 and H AC .…”
Section: Resultsmentioning
confidence: 94%
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“…As reported in ref. 13 , the value of 〈 m Λ 〉 varies markedly with 2 R in vortex-state spheres (〈 m Λ 〉 = 1 for single-domain spheres). In the present results, it was quite noticeable that the core reversal’s frequency is a function of both 〈 m Λ 〉 and H AC .…”
Section: Resultsmentioning
confidence: 94%
“…In the numerical calculation, we used 〈 m Λ 〉 = 73.6( l ex /2 R ) 2.20 with l ex the exchange length ( l ex ~ 5.3 nm for Py), as reported in ref. 13 . For the given material Py, f rev is therefore a function of both H AC and 2 R for the vortex-state spheres, but only of H AC for the single-domain spheres (i.e., 〈 m Λ 〉 = 1), independently of the particle size, as shown in the inset of Fig.…”
Section: Resultsmentioning
confidence: 99%
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