Determination of spin Hall angle in heavy metal/CoFeB-based heterostructures with interfacial spin-orbit fields
Witold Skowro\'nski, {\L}ukasz Karwacki, S{\l}awomir Zi\k{e}tek,, Jaros{\l}aw Kanak, Stanis{\l}aw {\L}azarski, Krzysztof Grochot, Tomasz, Stobiecki, Piotr Ku\'swik, Feliks Stobiecki, J\'ozef Barna\'s

TL;DR
This paper investigates spin Hall angles and interfacial spin-orbit fields in heavy metal/CoFeB heterostructures using SOT-FMR, revealing conditions for efficient magnetization switching through pure spin-current effects.
Contribution
It introduces an analytical model to determine spin Hall angles and interfacial spin-orbit fields, enhancing understanding of spin-current-induced magnetization dynamics in multilayers.
Findings
Spin Hall angle of -0.36 in W/CoFeB bilayers.
Spin Hall angle of 0.09 in CoFeB/Pt bilayers.
Interfacial spin-orbit fields can cancel Oersted fields, enabling pure spin-current dynamics.
Abstract
Magnetization dynamics in W/CoFeB, CoFeB/Pt and W/CoFeB/Pt multilayers was investigated using spin-orbit-torque ferromagnetic resonance (SOT-FMR) technique. An analytical model based on magnetization dynamics due to SOT was used to fit heavy metal (HM) thickness dependence of symmetric and antisymmetric components of the SOT-FMR signal. The analysis resulted in a determination of the properties of HM layers, such as spin Hall angle and spin diffusion length. The spin Hall angle of -0.36 and 0.09 has been found in the W/CoFeB and CoFeB/Pt bilayers, respectively, which add up in the case of W/CoFeB/Pt trilayer. More importantly, we have determined effective interfacial spin-orbit fields at both W/CoFeB and CoFeB/Pt interfaces, which are shown to cancel Oersted field for particular thicknesses of the heavy metal layers, leading to pure spin-current-induced dynamics and indicating the…
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