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Broadband Electron Spin Resonance Study in a Sr(2)FeMoO(6) Double Perovskite

[Image: see text] We report broadband magnetic resonance in polycrystalline Sr(2)FeMoO(6) measured over the wide temperature (T = 10–370 K) and frequency (f = 2–18 GHz) ranges. Sr(2)FeMoO(6) was synthesized by the sol–gel method and found to be ferromagnetic below T(C) = 325 K. A coplanar waveguide-...

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Detalles Bibliográficos
Autores principales: Das, Rajasree, Chaudhuri, Ushnish, Chanda, Amit, Mahendiran, Ramanathan
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7377272/
https://www.ncbi.nlm.nih.gov/pubmed/32715246
http://dx.doi.org/10.1021/acsomega.0c02070
Descripción
Sumario:[Image: see text] We report broadband magnetic resonance in polycrystalline Sr(2)FeMoO(6) measured over the wide temperature (T = 10–370 K) and frequency (f = 2–18 GHz) ranges. Sr(2)FeMoO(6) was synthesized by the sol–gel method and found to be ferromagnetic below T(C) = 325 K. A coplanar waveguide-based broadband spectrometer was used to record the broadband electron spin resonance (ESR) both in frequency sweep and field sweep modes. From the frequency sweep mode at fixed dc magnetic fields, we obtain the spectroscopic splitting factor g ∼ 2.02 for T ≥ T(C) K, which confirms the 3+ ionic state of Fe in the material. The effective g value was found to decrease monotonically with decreasing temperature in the ferromagnetic regime. Resonance frequency decreases and the line width of the spectra increases as the temperature decreases below T(C). At room temperature (RT) and above, the line width (ΔH) of the ESR signal increases linearly with frequency, giving Gilbert damping constant α ∼0.032 ± 0.005 at RT. However, at lower temperatures, a minimum emerges in the ΔH vs frequency curve, and the minimum shifts to a higher frequency with decreasing temperature, confining the linear frequency regime to a narrow-frequency regime. Additional inhomogeneous broadening and low-field-loss terms are needed to describe the line width in the entire frequency range.