Abstract

Iridium is a very promising material for spintronic applications due to its interesting magnetic properties such as large RKKY exchange coupling as well as its large spin-orbit coupling value. Ir is for instance used as a spacer layer for perpendicular synthetic antiferromagnetic or ferrimagnet systems. However, only a few studies of the spintronic parameters of this material have been reported. In this paper, we present inverse spin Hall effect - spin pumping ferromagnetic resonance measurements on CoFeB/Ir based bilayers to estimate the values of the effective spin Hall angle, the spin diffusion length within iridium, and the spin mixing conductance in the CoFeB/Ir bilayer. In order to have reliable results, we performed the same experiments on CoFeB/Pt bilayers, which behavior is well known due to numerous reported studies. Our experimental results show that the spin diffusion length within iridium is 1.3 nm for resistivity of 250 n$\Omega$.m, the spin mixing conductance $g_{eff}^{\uparrow \downarrow}$ of the CoFeB/Ir interface is 30 nm$^{-2}$, and the spin Hall angle of iridium has the same sign than the one of platinum and is evaluated at 26% of the one of platinum. The value of the spin Hall angle found is 7.7% for Pt and 2% for Ir. These relevant parameters shall be useful to consider Ir in new concepts and devices combining spin-orbit torque and spin-transfer torque.

Highlights

  • Iridium is a very promising material for spintronic applications

  • We can use the remark from Ref. [26], stating that in the case of Pt, given the results reported in the literature, the product of the effective spin Hall angle and the spin diffusion length, θSH × ls f, is a quantity that is nearly independent of the technique or the setup used, and its effective value is estimated to be close to 0.19 nm

  • We have described an approach that enables the measurement of the spin Hall angle of a material with respect to another one

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Summary

INTRODUCTION

Iridium is a very promising material for spintronic applications. Its properties include large spin-orbit coupling [1], large Ruderman-Kittel-Kasuya-Yosida (RKKY) exchange coupling [2], and strong interface contribution to perpendicular magnetic anisotropy (PMA) [3,4,5,6] and to interfacial Dzyaloshinskii-Moriya interaction [7]. From the peaks at resonance, several materials properties can be deduced From this ISHE spin pumping voltage, the resonance magnetic field Hres as a function of the frequency f of the rf excitation applied to the sample gave us information about the ferromagnetic layer excited. The relationship between these parameters is described by the Kittel law [36], as presented in Fig. 2(b): f. From the measurement of the spin pumping voltage as a function of the applied field [Fig. 2(a)] one can determine the linewidth H of the voltage peaks to estimate the magnetic damping α of the materials.

Our results show consistent values of r f
The obtained value
Ir SP
SHE efficiencies to be θSIHr θSPHt
Findings
CONCLUSION
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