2021
DOI: 10.1016/j.jmmm.2021.167945
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General approach for anisotropic magnetoresistance calculations used for revealing the role of cobalt nanowire’s geometrical details

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Cited by 2 publications
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“…The mesh size of the 2D system was fixed at 4 × 4 nm 2 , which is lower than the exchange length of cobalt (∼5 nm). 44 The temperature was set as 300 K. The saturation magnetization and exchange stiffness constant A were chosen to be 8.70 × 10 5 A•m −1 and 1.66 × 10 −11 J•m −1 , respectively. The initial magnetization state was set to be a stripe domain structure.…”
Section: Methodsmentioning
confidence: 99%
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“…The mesh size of the 2D system was fixed at 4 × 4 nm 2 , which is lower than the exchange length of cobalt (∼5 nm). 44 The temperature was set as 300 K. The saturation magnetization and exchange stiffness constant A were chosen to be 8.70 × 10 5 A•m −1 and 1.66 × 10 −11 J•m −1 , respectively. The initial magnetization state was set to be a stripe domain structure.…”
Section: Methodsmentioning
confidence: 99%
“…A 2 × 2 μm 2 two-dimensional (2D) system of 12 repetitions of a trilayer stack consisting of Pt (3 nm), Co (1.7 nm), and Ta (2.3 nm) was used with applying the 2D periodic boundary conditions. The mesh size of the 2D system was fixed at 4 × 4 nm 2 , which is lower than the exchange length of cobalt (∼5 nm) . The temperature was set as 300 K. The saturation magnetization and exchange stiffness constant A were chosen to be 8.70 × 10 5 A·m –1 and 1.66 × 10 –11 J·m –1 , respectively.…”
Section: Methodsmentioning
confidence: 99%