2015
DOI: 10.1063/1.4906062
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Quantification of the spin-Hall anti-damping torque with a resonance spectrometer

Abstract: We present a simple technique using a cavity-based resonance spectrometer to quantify the anti-damping torque due to the spin Hall effect. Modification of ferromagnetic resonance is observed as a function of small DC current in sub-mm-wide strips of bilayers, consisting of magnetically soft FeGaB and strong spin-Hall metal Ta. From the detected current-induced linewidth change, we obtain an effective spin Hall angle of 0.08-0.09 independent of the magnetic layer thickness. Our results demonstrate that a sensit… Show more

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Cited by 16 publications
(16 citation statements)
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“…This effect was first predicted by Dyakonov and Perel 3 , where due to spin-orbit interaction 18 an electrical current results in transverse flow of spins with polarisation perpendicular to both the charge and spin current directions 19 . The SHE was demonstrated using a number of techniques, including field-swept ferromagnetic resonance (FMR) 20 , 21 , spin torque FMR 22 24 , optical FMR 25 , time-resolved optical techniques 26 and electrical methods 27 . The SHE-generated spin polarisation results in a torque when injected in a ferromagnetic layer, which makes this effect very important for magnetic devices, resulting in motion of domain walls 28 with important applications to synthetic antiferromagnetic domain wall devices 29 , 30 .…”
Section: Introductionmentioning
confidence: 99%
“…This effect was first predicted by Dyakonov and Perel 3 , where due to spin-orbit interaction 18 an electrical current results in transverse flow of spins with polarisation perpendicular to both the charge and spin current directions 19 . The SHE was demonstrated using a number of techniques, including field-swept ferromagnetic resonance (FMR) 20 , 21 , spin torque FMR 22 24 , optical FMR 25 , time-resolved optical techniques 26 and electrical methods 27 . The SHE-generated spin polarisation results in a torque when injected in a ferromagnetic layer, which makes this effect very important for magnetic devices, resulting in motion of domain walls 28 with important applications to synthetic antiferromagnetic domain wall devices 29 , 30 .…”
Section: Introductionmentioning
confidence: 99%
“…A high-impedance current source outputs I dc , and we restrict |I dc | ≤ 2 mA (equivalent to the current density in Pt |J c,P t | < 10 11 A/m 2 ) to minimize Joule heating and nonlinear dynamics. The dependence of the resonance linewidth W on I dc allows for quantification of the damping-like torque 48,[54][55][56][57][58][59][60] , while the change in the resonance field H F MR yields a direct measure of the field-like torque 52 . Thus, dc-tuned ST-FMR quantifies both spinorbit torque contributions.…”
Section: B Spin-torque Ferromagnetic Resonancementioning
confidence: 99%
“…60. These NiFe/(Cu/)Pt strips were fabricated on the same substrate as the ST-FMR device sets described in Sec.…”
Section: Electrical Detection Of Spin Pumpingmentioning
confidence: 99%
“…There have been many other techniques developed over the last decade, although are less popular but utilize interesting phenomena in probing SOTs or estimating the charge-spin conversion efficiency. Notable among them are the SHE tunneling spectroscopy proposed by Liu et al, 79 resonance spectroscopy by Emori et al, 80 longitudinal magneto-optic Kerr effect (MOKE) method by Fan et al, 36 SHE-driven chiral domain wall motion technique by Emori et al, 66 and thermal injection method by Qu et al 81 As a final remark, we address the challenges that these existing quantification techniques might face while the systems-of-interests are heterostructures with emergent materials such as TIs, TMDs, and Weyl semimetals. First of all, unlike conventional metallic SH layers, these exotic materials, such as Bi2Se3, 37,[82][83][84] (Bi0.5Sb0.5)2Te3, 85,86 WTe2, 87,88 and MoTe2 [89][90][91] are typically highly resistive (𝜌 SH > 10 2 μΩ-cm).…”
Section: Discussionmentioning
confidence: 99%