2016
DOI: 10.1103/physrevb.94.224423
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Spin transport and dynamics in all-oxide perovskite La2/3Sr1/3MnO3/SrRuO3

Abstract: Thin films of perovskite oxides offer the possibility of combining emerging concepts of strongly correlated electron phenomena and spin current in magnetic devices. However, spin transport and magnetization dynamics in these complex oxide materials are not well understood. Here, we experimentally quantify spin transport parameters and magnetization damping in epitaxial perovskite ferromagnet/paramagnet bilayers of La 2/3 Sr 1/3 MnO3/SrRuO3 (LSMO/SRO) by broadband ferromagnetic resonance spectroscopy. From the … Show more

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Cited by 47 publications
(29 citation statements)
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“…In this fitting, we take into account the thickness dependence of the SrIrO 3 resistivity which increases in ultrathin films due to scattering mechanisms (see SI Appendix for details), which gives a spin-mixing conductance G ↑↓ of 1.8 × 10 14 Ω −1 •m −2 and a spin diffusion length of 1.4 nm. These are consistent with that reported in the LaSrMnO 3 /SrRuO 3 system (47). The value of the spin-diffusion length corresponds to the tetragonal phase of SrIrO 3 , since the damping parameter is largely saturated already for thicknesses less than the point of transition to the orthogonal phase at 4.8 nm (12 uc).…”
Section: Methodssupporting
confidence: 89%
“…In this fitting, we take into account the thickness dependence of the SrIrO 3 resistivity which increases in ultrathin films due to scattering mechanisms (see SI Appendix for details), which gives a spin-mixing conductance G ↑↓ of 1.8 × 10 14 Ω −1 •m −2 and a spin diffusion length of 1.4 nm. These are consistent with that reported in the LaSrMnO 3 /SrRuO 3 system (47). The value of the spin-diffusion length corresponds to the tetragonal phase of SrIrO 3 , since the damping parameter is largely saturated already for thicknesses less than the point of transition to the orthogonal phase at 4.8 nm (12 uc).…”
Section: Methodssupporting
confidence: 89%
“…The in-plane angular dependence of the FMR linewidth can be analyzed by considering the different contributions: [36][37][38][39] Gilbert damping, two-magnon scattering, linewidth broadening due to mosaicity, and inhomogeneous linewidth broadening. The inhomogeneous linewidth broadening caused by the fluctuation of the strength of the anisotropy fields is angle independent.…”
Section: Fmr Measurement Resultsmentioning
confidence: 99%
“…где H Pt/YIG -ширина линии FMR гетероструктуры Pt/YIG. При однородном уширении линии поглощения g ↑↓ экспериментально определяется утечкой спинов через границу [3,5,8,10]:…”
Section: спиновая проводимость границы Pt/yigunclassified