Abstract

We report ferromagnetic resonance (FMR) experiments on thin magnetic Co layers either sandwiched symmetrically between Cu and Pt, or sandwiched asymmetrically between a Cu or Pt layer on one side and a ${\mathrm{SiO}}_{x}$ substrate on the other. In the symmetric samples, we find well-known behavior, namely, the FMR linewidth $\ensuremath{\Delta}{H}_{pp}$ is significantly larger for the case of Pt than for the case of Cu. This is due to the larger spin scattering in the Pt layer. However, for the asymmetric Co/Cu bilayers, the linewidth is much larger than for the symmetric Cu/Co/Cu trilayers and not much different from the linewidth of Co/Pt bilayers. We argue this to be due to the Rashba effect at the ${\mathrm{SiO}}_{x}/\mathrm{Co}$ interface, which gives rise to effective magnetic fields interacting with the electron spins in the Co layer and which can be measured without reverting to transport measurements.

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