Abstract

The emergence of spin-orbit torques as a promising approach to energy-efficient magnetic switching has generated large interest in material systems with easily and fully tunable spin-orbit torques. Here, current-induced spin-orbit torques in VO2_2/NiFe heterostructures were investigated using spin-torque ferromagnetic resonance, where the VO2_2 layer undergoes a prominent insulator-metal transition. A roughly two-fold increase in the Gilbert damping parameter, αα, with temperature was attributed to the change in the VO2_2/NiFe interface spin absorption across the VO2_2 phase transition. More remarkably, a large modulation (±\pm100%) and a sign change of the current-induced spin-orbit torque across the VO2_2 phase transition suggest two competing spin-orbit torque generating mechanisms. The bulk spin Hall effect in metallic VO2_2, corroborated by our first-principles calculation of spin Hall conductivity, σSH≈104ℏeΩ−1m−1σ_{SH} \approx 10^4 \frac{\hbar}{e} Ω^{-1} m^{-1}, is verified as the main source of the spin-orbit torque in the metallic phase. The self-induced/anomalous torque in NiFe, of the opposite sign and a similar magnitude to the bulk spin Hall effect in metallic VO2_2, could be the other competing mechanism that dominates as temperature decreases. For applications, the strong tunability of the torque strength and direction opens a new route to tailor spin-orbit torques of materials which undergo phase transitions for new device functionalities.

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