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Efficient spin-orbit torque (SOT) switching is of crucial importance for magnetic random-access memory. In this work, we study the SOT switching of ferrimagnetic alloy, which permits ultrafast switching in picoseconds. We find that the magnetization is first reversed at the corner of the sample, which then propagates to the entire sample through domain-wall motion. We show that the location of this corner exhibits both left-right and top-down asymmetry, and it is uniquely determined by the polarity of current and external field (Hx). In the ferromagnetic system, previous studies have concluded that the top-down asymmetry is induced by the field-like SOT, which is absent in our system. We propose that the damping-like SOT, Dzyaloshinskii-Moriya interaction, and Hx are sufficient to explain the findings. This work improves our understanding of the physics behind the SOT switching.
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