2011
DOI: 10.1016/j.jmmm.2010.10.002
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Compressed exponential form for disordered domain wall motion in ultra-thin Au/Co/Au ferromagnetic films

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Cited by 21 publications
(10 citation statements)
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“…3(a), it can be concluded that the magnetization reversal is dominated by domain wall motion. 21 As the time was increased the number of domain nucleation sites increases as confirmed by the domain images for h ¼ 60 shown in Figs. 4(a) and 4(b).…”
Section: Resultsmentioning
confidence: 68%
See 1 more Smart Citation
“…3(a), it can be concluded that the magnetization reversal is dominated by domain wall motion. 21 As the time was increased the number of domain nucleation sites increases as confirmed by the domain images for h ¼ 60 shown in Figs. 4(a) and 4(b).…”
Section: Resultsmentioning
confidence: 68%
“…where M 0 þ M 1 is the normalized saturation magnetization, s is the relaxation time obtained from the fit, and b > 1 a compressing exponent as introduced by Adjanoh et al 21 Here, the very fast dynamics (<1 s) of the initial switching from À(M 0 þ M 1 ) to þM 0 has not been taken into account. From the fittings using Eq.…”
Section: Resultsmentioning
confidence: 99%
“…Here the normalized intensity as a function of time basically reflects the net magnetization relaxation of the sample. Amongst various raised models to explain magnetization relaxation phenomena Fatuzzo-Labrune model is extensively used for FM thin films [38][39][40][41][42][43]. However, the approximation of single energy barrier made in this model does not hold for a real thin film which consists of a distribution of energy barrier with defects and inhomogeneity throughout the surface.…”
Section: Relaxation Dynamicsmentioning
confidence: 99%
“…The last model can be rewritten in terms of the competition between domain nucleation and domain-wall (DW) motion [34,[36][37][38]:…”
Section: B Competition Between Domain Nucleation and Domain-wall Promentioning
confidence: 99%