The resonant frequency for this case can be represented as an analytical function: ω2 r =κ 1κ2 − (κ3 −κ 4)2 4 ,(C6)

+κ 1κ6(κ3 +κ 4) i ω2 r =κ 1κ2 − (κ3 −κ 4)2 4 ,(C5) whereξ 2 1 =κ 1κ2 +κ 3κ4,ξ 2 2 =κ 2κ5 −κ 3κ6 andξ 2 3 =κ 4κ5 +κ 1κ6

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cond-mat.mtrl-sci · 2026-04-08 · unverdicted · novelty 6.0 · 2 refs

Linearly polarized light shifts ferromagnetic resonance frequency through the inverse Cotton-Mouton effect and can dominate thermal shifts.

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Optomagnetic non-thermal modification of the ferromagnetic resonance cond-mat.mtrl-sci · 2026-04-08 · unverdicted · none · ref 2 · 2 links
Linearly polarized light shifts ferromagnetic resonance frequency through the inverse Cotton-Mouton effect and can dominate thermal shifts.