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Nonlocal Interaction of Inverse Magnetic Energy Transfer in Hall Magnetohydrodynamic Turbulence

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Figure

Fig. 1. To compare the various time results, all the abscis-(b)(t)�bers k (t) :�4(u)(t)�3, k (t) :3 ⃗for the magnetic field, respectively
Fig. 2 (b)). Energy is absorbed around k/kη≃ 0.transferred to the smaller wave number region k/k(b)(b)η
Fig. 4Normalized wavelet-scale spectra of the Hall term effect�bk���b���b�Hall. Ordinates are normalized by the magneticdissipation rate ϵ(b).
Fig. 5Typical wavelet-scale triad interaction profiles caused by �b���b���b�

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