2010
DOI: 10.1016/j.jmmm.2009.09.039
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Magnetic anisotropy and spin reorientation in Co/Pt multilayers: Influence of preparation

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Cited by 25 publications
(15 citation statements)
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“…The first reason is the gradual reduction of the thickness of the Co layer as below t Co ≲ 0.5 nm the first order anisotropy constant K 1,eff decreases with decreasing t Co . 41 This behavior is in accordance with other studies, see, e.g., Refs. 42,43.…”
Section: Resultssupporting
confidence: 93%
“…The first reason is the gradual reduction of the thickness of the Co layer as below t Co ≲ 0.5 nm the first order anisotropy constant K 1,eff decreases with decreasing t Co . 41 This behavior is in accordance with other studies, see, e.g., Refs. 42,43.…”
Section: Resultssupporting
confidence: 93%
“…Below t c , the K eff saturates at 0.25 6 0.03 mJ/m 2 , likely due to the decrease of interfacial anisotropy ascribed to the degradation of the interfaces when the Co thickness decreases. 39,40 This is comparable to values reported in the literature for similar Co-Pt thin film stacks, 3,4 which are on the order of 0.3-0.32 mJ/m 2 . An increased annealing temperature has been reported to decrease the K eff .…”
Section: B Magnetic Characterizationsupporting
confidence: 88%
“…One possible explanation is that the out-of-plane component of the magnetization is reduced. Such behavior can be expected within the spin-reorientation transition when magnetization canting is effective [21,30,31,[47][48][49]. In addition, the fit via the model reveals that the shape parameter has to be changed from k = 4 to 3.3 [ Fig.…”
Section: Scattering Model For the Maze Patternmentioning
confidence: 94%
“…First, seed layers of 4-nm Pt (plasma-based ion-beam sputtering) and 3.5-nm Pd (dc magnetron sputtered) are grown. On the seed layer, the Co/Pd multilayer stack is deposited (dc magnetron sputtered) and capped by a 3.5-nm Pd layer [29][30][31] [ Fig. 1(b)].…”
Section: Methodsmentioning
confidence: 99%