2017
DOI: 10.1103/physrevb.95.060409
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Parametric frequency mixing in a magnetoelastically driven linear ferromagnetic-resonance oscillator

Abstract: We demonstrate the nonlinear frequency conversion of ferromagnetic resonance (FMR) frequency by optically excited elastic waves in a thin metallic film on dielectric substrates. Time-resolved probing of the magnetization directly witnesses magneto-elastically driven second harmonic generation, sum-and difference frequency mixing from two distinct frequencies, as well as parametric downconversion of each individual drive frequency. Starting from the Landau-Lifshitz-Gilbert equations, we derive an analytical equ… Show more

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Cited by 40 publications
(41 citation statements)
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“…They can be generated [11] and controlled [12] optically via the excitation of transient gratings (TGs) [13,14]. Recently, these TG-excitations heave been used to probe heat transport in suspended thin films [15] and magneto-elastic coupling in thin nickel films [16][17][18]. Optical excitation of a solid generates not only coherent sound waves but also incoherent thermal strain.…”
mentioning
confidence: 99%
“…They can be generated [11] and controlled [12] optically via the excitation of transient gratings (TGs) [13,14]. Recently, these TG-excitations heave been used to probe heat transport in suspended thin films [15] and magneto-elastic coupling in thin nickel films [16][17][18]. Optical excitation of a solid generates not only coherent sound waves but also incoherent thermal strain.…”
mentioning
confidence: 99%
“…where, λ a is the array repeat period (λ a = 500nm), f saw is the frequency of the optically excited SAW, as measured from the experimental data (f saw = 6GHz), B ∼ 7.85M J/m 3 and xx ∼ 200ppm 19 . While we believe the experimental strains to be larger than this value, micromagnetic simulations were conducted at this reduced strain to ensure linearity of the simulated results, while the experimental results do not show responses that would be associated with frequency mixing phenomena we reported previously 39 . The anisotropy axis is applied along the x-axis of the array.…”
Section: Resultsmentioning
confidence: 99%
“…2 under the influence of the magnetostriction and the damping effect, from the macrospin model. Unlike ( 30 , 31 ), the role of backaction is included, which allows predictions for the experimentally observed hybridization. We define that the z ′ axis is titled from the original z axis with an angle and perpendicular to the original x axis.…”
Section: Methodsmentioning
confidence: 99%