2020
DOI: 10.35848/1882-0786/abc6eb
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Reduction of back switching by large damping ferromagnetic material

Abstract: Recent studies on magnetization dynamics induced by spin-orbit torque have revealed a weak dependence of the critical current for magnetization switching on the damping constant of a ferromagnetic free layer. This study, however, reveals that the damping constant nevertheless plays a key role in magnetization switching induced by spin-orbit torque. An undesirable switching, returning to an initial state, named as back switching, occurs in a ferromagnet with an easy axis parallel to the current direction. Numer… Show more

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Cited by 3 publications
(2 citation statements)
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References 36 publications
(83 reference statements)
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“…We notice that the auto-oscillation is excited when β is positive. In fact, auto-oscillations have not been observed in this geometry when the field-like torque is absent [24,45,46] or β is negative [29]. This argument is also confirmed from the critical-current formula to excite the auto-oscillation shown in supplementary material, where the critical current is inversely proportional to √ β, and therefore, becomes finite only for a finite β.…”
supporting
confidence: 71%
“…We notice that the auto-oscillation is excited when β is positive. In fact, auto-oscillations have not been observed in this geometry when the field-like torque is absent [24,45,46] or β is negative [29]. This argument is also confirmed from the critical-current formula to excite the auto-oscillation shown in supplementary material, where the critical current is inversely proportional to √ β, and therefore, becomes finite only for a finite β.…”
supporting
confidence: 71%
“…For a pulse shut off at 4.8 ns, when the average m z exactly passes the x-axis, the magnetization goes through a period of oscillation around the hard axis in the x-y plane and finally relaxes to the other side, as labeled by the red line in figure 4(a). This anomalous phenomenon, which might be attributed to relatively weak anisotropy field, implies the possible risk of back switching, as mentioned by the researchers [57,58], and thus for clarity, the switching time is regarded as the time that the average m z reaches −0.9. For a pulse width longer than 5 ns, the magnetization relaxes to the other side after the pulse shuts off and the switching time is shortened along with the pulse width increasing.…”
mentioning
confidence: 99%