Orbital torque of Cr-induced magnetization switching in perpendicularly magnetized Pt/Co/Pt/Cr heterostructures

Abstract

The spin-orbit torque via the spin Hall effect of heavy metals has shown promising prospect in driving the magnetization switching in spintronic devices due to the generated spin current from heavy metals. Recently, the 3d-light metals have been predicted the ability to generate orbital current and the associated orbital torques from the orbital Hall effect. However, few experiments have been carried out since it’s quite hard to directly detect the orbital current generated orbital torque. Here, we report an effective method to demonstrate the strong orbital torques in light metal Cr through a conversion process from orbital current to spin current by introducing the Pt interfacial layer in perpendicular magnetized symmetric Pt/Co/Pt structures. A quite large and monotonically growth of orbital torque efficiency in Pt/Co/Pt/Cr with the increase of the thickness of Cr layer is obtained with the largest effective orbital torque efficiency around 2.6 Oe/(MA·cm-2). The ability of orbital torque to drive the magnetization switching is also reported with the critical switching current density down to the order of 106 A·cm-2. Our findings prove the efficiency for switching the magnetization from light metal Cr layers through the orbital Hall effect.

Spin transport characteristics modulated by the GeBi interlayer in Y3Fe5O12/GeBi/Pt heterostructures

“…[1,2] The main challenges in the development of modern semiconductor spintronics are the generation, detection, and manipulation of spin currents. [3][4][5][6][7][8][9][10] The manipulation of a pure spin current results in low-cost energy and high-efficiency electronics. Compared with the traditional spin-injection method that introduces a spin-polarized charge current, [11][12][13][14][15] in a ferromagnet (FM)/nonmagnetic (NM) material structure, ferromagnetic resonance (FMR)-driven spin pumping can generate a pure spin current without a charge current via the angular momentum transfer from FM to NM material.…”