Fig. 3

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Resonance amplification factor, W, vs. frequency of oscillation, ω (solid red line). The vertical dashed violet line marks the resonance peak at ω = ωres, and the dashed green line indicates the frequency of the tidal potential component that is responsible for exciting the oscillations, ωmn. When the magnetic field, B, of the flux tube increases, the resonance peak moves toward the right because ωres increases. On the contrary, when the magnetic field strength decreases, the peak moves toward the left. Therefore, the perturbationΔB2 produced by the oscillation displacement, ξr, can lock the system into resonance, with ωmn being slightly greater than ωres, as illustrated (see text).
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