2020
DOI: 10.1016/j.jmmm.2020.166929
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Magnetization states driven by spin-transfer torque in spin-valve nanopillars in presence of four-fold magnetocrystalline anisotropy

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Cited by 4 publications
(1 citation statement)
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“…The dynamics of the AFM skyrmion is realized by applying a current density through the HM, generating SOTs in the AFM layer. The equation describing the skyrmion dynamics driven by SOTs is given by , normald m i normald t = prefix− γ 0 ( bold-italicm bold-italici × bold-italicH boldeff ) + α ( m i × normald m i normald t ) γ 0 m i × ( m i × θ SHE J HM 2 μ 0 e M s d e y ) Here, m i represents the normalized magnetization, H eff is the effective field, γ is the gyromagnetic ratio, α is the Gilbert damping, θ SHE is the spin Hall angle (SHA), J HM is the pulsed current density flowing in the negative x -axis along the HM layer, μ 0 is the vacuum permeability, e is the elementary electron charge, M s is the saturation magnetization, and d is the AFM layer thickness.…”
Section: Simulation Methodsmentioning
confidence: 99%
“…The dynamics of the AFM skyrmion is realized by applying a current density through the HM, generating SOTs in the AFM layer. The equation describing the skyrmion dynamics driven by SOTs is given by , normald m i normald t = prefix− γ 0 ( bold-italicm bold-italici × bold-italicH boldeff ) + α ( m i × normald m i normald t ) γ 0 m i × ( m i × θ SHE J HM 2 μ 0 e M s d e y ) Here, m i represents the normalized magnetization, H eff is the effective field, γ is the gyromagnetic ratio, α is the Gilbert damping, θ SHE is the spin Hall angle (SHA), J HM is the pulsed current density flowing in the negative x -axis along the HM layer, μ 0 is the vacuum permeability, e is the elementary electron charge, M s is the saturation magnetization, and d is the AFM layer thickness.…”
Section: Simulation Methodsmentioning
confidence: 99%