Temperature Evolution of Magnon Propagation Length in Tm${}_3$Fe${}_5$O${}_{12}$ Thin Films: Roles of Magnetic Anisotropy and Gilbert Damping

Abstract

The magnon propagation length ($⟨\xi ⟩$) of a ferro/ferrimagnet (FM) is one of the key factors that controls the generation and propagation of thermally-driven spin current in FM/heavy metal (HM) bilayer based spincaloritronic devices. Theory predicts that for the FM layer, $⟨\xi ⟩$ is inversely proportional to the Gilbert damping ($\alpha$) and the square root of the effective magnetic anisotropy constant ($K_{\mathrm{eff}}$). However, direct experimental evidence of this relationship is lacking. To experimentally confirm this prediction, we employ a combination of longitudinal spin Seebeck effect (LSSE), transverse susceptibility, and ferromagnetic resonance experiments to investigate the temperature evolution of $⟨\xi ⟩$ and establish its correlation with the effective magnetic anisotropy field, $H_K^{\mathrm{eff}}$ ($\propto K_{\mathrm{eff}}$) and $\alpha$ in Tm${}_3$Fe${}_5$O${}_{12}$ (TmIG)/Pt bilayers. We observe concurrent drops in the LSSE voltage and $⟨\xi ⟩$ below 200${}^{\circ }$K in TmIG/Pt bilayers regardless of TmIG film thickness and substrate choice and attribute it to the noticeable increases in $H_K^{\mathrm{eff}}$ and $\alpha$ that occur within the same temperature range. From the TmIG thickness dependence of the LSSE voltage, we determined the temperature dependence of $⟨\xi ⟩$ and highlighted its correlation with the temperature-dependent $H_K^{\mathrm{eff}}$ and $\alpha$ in TmIG/Pt bilayers, which will be beneficial for the development of rare-earth iron garnet-based efficient spincaloritronic nanodevices.

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