Switching of perpendicularly magnetized nanomagnets with spin-orbit torques in the absence of external magnetic fields

Abstract

A method of controlling a trajectory of a perpendicular magnetization switching of a ferromagnetic layer using spin-orbit torques in the absence of any external magnetic field includes: injecting a charge current J e through a heavy-metal thin film disposed adjacent to a ferromagnetic layer to produce spin torques which drive a magnetization M out of an equilibrium state towards an in-plane of a nanomagnet; turning the charge current J e off after t e seconds, where an effective field experienced by the magnetization of the ferromagnetic layer H eff is significantly dominated by and in-plane anisotropy H kx , and where M passes a hard axis by precessing around the H eff ; and passing the hard axis, where H eff is dominated by a perpendicular-to-the-plane anisotropy H kz , and where M is pulled towards the new equilibrium state by precessing and damping around H eff , completing a magnetization switching.

What is claimed is: 
     
         1 . A method of controlling a trajectory of a perpendicular magnetization switching of a ferromagnetic layer using spin-orbit torques in the absence of any external magnetic field comprising:
 injecting a charge current J e  through a heavy-metal thin film disposed adjacent to a ferromagnetic layer to produce spin torques which drive a magnetization M out of an equilibrium state towards an in-plane of a nanomagnet;   turning said charge current J e  off after t e  seconds, causing a spin torque to reduce to substantially zero where M is close to an x-y plane and away from an e z  axis by an angle of ϑ in a critical zone, where an effective field experienced by the magnetization of the ferromagnetic layer H eff  is significantly dominated by and in-plane anisotropy H kx , and where M passes a hard axis by precessing around said H eff ; and   passing the hard axis, where H eff  is dominated by a perpendicular-to-the-plane anisotropy H kz , and where M is pulled towards the new equilibrium state by precessing and damping around H eff , completing a magnetization switching.   
     
     
         2 . The method of  claim 1 , wherein a duration of said t e  of an applied current pulse comprises a shortest time which causes said magnetization M to move from said equilibrium state to said critical zone.