2011
DOI: 10.1007/s11433-011-4313-1
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Magnetization switching modes in nanopillar spin valve under the external field

Abstract: The current-induced magnetic switching is studied in Co/Cu/Co nanopillar with an in-plane magnetization traversed under the perpendicular-to-plane external field. Magnetization switching is found to take place when the current density exceeds a threshold. By analyzing precessional trajectories, evolutions of domain walls and magnetization switching times under the perpendicular magnetic field, there are two different magnetization switching modes: nucleation and domain wall motion reversal; uniform magnetizati… Show more

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Cited by 8 publications
(5 citation statements)
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“…The details for obtaining E k , E d , E ext , and E ex can be found in our previous papers. [36][37][38] Note that a finite size magnet magnetostatic boundary condition 39 is applied to calculate the demagnetization energy E d , to consider the influence of geometric size on the magnetic domain structures of such three-dimensional nanomagnets.…”
mentioning
confidence: 99%
“…The details for obtaining E k , E d , E ext , and E ex can be found in our previous papers. [36][37][38] Note that a finite size magnet magnetostatic boundary condition 39 is applied to calculate the demagnetization energy E d , to consider the influence of geometric size on the magnetic domain structures of such three-dimensional nanomagnets.…”
mentioning
confidence: 99%
“…The dynamics of magnetization is investigated by numerically solving the timedependent LLGS equation using the Gauss-Seidel projection method with a constant time step ∆t= 0.0268858 ps. [36][37][38] We adopted the following magnetic parameters, magnetocrystalline anisotropy constant K 1 =3.0×10 3 J/m 3 , and K 2 =0, 39 exchange constant A=2.0×10 -11 J/m, 40 saturation magnetization M s =8.0×10 5 A/m. 41 Other parameters are Gilbert damping parameter α=0.008, 14 spin polarization factor η=0.56, 42,43 electron gyromagnetic ratio γ=2.3245×10 5 For clarify, the PSD of y axis shifts up with 0.5 each curve with the increase of external stress.…”
Section: Methodsmentioning
confidence: 99%
“…29 The initial magnetizations of free and pinned layers are along the Àx axis and þx axis, respectively. The dynamics of magnetization was investigated by numerically solving the time-dependent LLGS equation using the Gauss-Seidel projection method [33][34][35][36] with a constant time step Dt ¼ 0.0238993 ps. The samples were discrete in computational cells of 2 Â 2 Â 2 nm 3 .…”
Section: Model Descriptionmentioning
confidence: 99%