Fig. 9.

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Real and imaginary parts of ω for a standing ion-acoustic wave derived from hybrid simulations as a function of the amplitude of the Alfvénic pump. For the top curve βe = 6 × 10−2 and βp = 10−2, while for the bottom curve βe = 10−1 and βp = 1.25 × 10−2. In this simulation k0 = 2π/L. The attenuation is calculated from the Fourier analysis in space and the power of the mode m′ = 2 (or m = 4). The horizontal dashed line corresponds to the expected real and imaginary frequency of the corresponding non-driven ion-acoustic mode attenuated by LD and calculated from the numerical solution of Eq. (19).
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