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technical paper
Spin Orbit Torque Induced Ultrafast Magnetization Switching in a Ferromagnet
Spin-orbit-torque (SOT) based magnetic devices1 have gained considerable attention due to their non-volatility, speed, and energy efficiency. SOT-induced magnetization switching studies are limited by the rise-time and duration of available pulsed current sources 2,3. Recently, ultrafast SOT switching has been demonstrated using ~ps current pulses4,obtained from an optically excited photoconductive (Auston) switch4,5, although the switching dynamics have not yet been reported. Here, we report the ultrafast magnetization dynamics measured via the time-resolved polar magneto-optical Kerr effect (MOKE)5
in a ferromagnet (inset of Fig. 1), using the ultrafast SOT
effect due to a ~ 9 ps long current pulse generated from an Auston switch. The ~ps current pulse, without any in-plane magnetic field, introduces a demagnetization of ~30% and softens the magnet at an ultrafast timescale. In the presence of a 1600 Oe symmetry-breaking in-plane field, SOT tries to rotate the magnetic moments away from the saturation state, for a negative
current pulse (blue line in Fig. 1), which when combined with the ultrafast demagnetization, shows a reduced initial demagnetization coupled with SOT-oscillations at longer timescales.
However, for positive current, it induces a coherent rotation of the softened magnetic moments toward the negative saturation. Magnetization crosses zero in ~65 ps and switches fully after
about ~200 ps (red line in Fig. 1). Sub-ns current pulse-induced SOT dynamics are governed by domain-wall propagation with an additional incubation delay due to domain nucleation 6-8.
The absence of any incubation delay combined with the fast-switching time leads us to believe that the switching is probably governed by the coherent rotation of the softened magnetic
moment due to ultrafast heating by the ~ps current pulse excitation. A micromagnetic simulation coupled with 2-temperature ultrafast heating qualitatively agrees well with the observed dynamics (dotted lines in Fig. 1). Our work sheds significant insights on the mechanism of picosecond SOT-induced magnetization dynamics.
References
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Fig. 1. Ultrafast magnetization dynamics with positive and negative ~ps current pulse direction. The theoretical analysis is shown in dotted lines.