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Broadband Electron Spin Resonance Study in a Sr2FeMoO6 Double Perovskite
Author(s) -
Rajasree Das,
Ushnish Chaudhuri,
Amit Chanda,
R. Mahendiran
Publication year - 2020
Publication title -
acs omega
Language(s) - Uncategorized
Resource type - Journals
SCImago Journal Rank - 0.779
H-Index - 40
ISSN - 2470-1343
DOI - 10.1021/acsomega.0c02070
Subject(s) - ferromagnetic resonance , condensed matter physics , electron paramagnetic resonance , resonance (particle physics) , materials science , atmospheric temperature range , full width at half maximum , ferromagnetism , crystallite , nuclear magnetic resonance , atomic physics , analytical chemistry (journal) , magnetic field , chemistry , physics , magnetization , optoelectronics , meteorology , metallurgy , quantum mechanics , chromatography
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 (Δ H ) 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 Δ H 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.

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