Fig. 8.

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Kinetic and magnetic horizontally integrated energy spectra during the saturation phase obtained with ℓmax = 128 for simulation run B. Opaque lines represent the spectra excluding ℓ = 0 components, while transparent lines include them. The oscillations visible at high k/kR when including ℓ = 0 components result from the our direct integration of Eq. (A.5) which involves spherical Bessel functions jℓ(kr) that are very oscillatory for kr ≫ ℓ.
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