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Fig. 9.

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Left panel: Normalized power spectra of the velocity E K ( ) = E K ( ) / l E K ( ) $ \tilde{E}_{\mathrm{K}}^{(\ell)} = E_{\mathrm{K}}^{(\ell)}/ \sum_l E_{\mathrm{K}}^{(\ell)} $ and magnetic fields E M ( ) = E M ( ) / l E K ( ) $ \tilde{E}_{\mathrm{M}}^{(\ell)} = E_{\mathrm{M}}^{(\ell)}/ \sum_l E_{\mathrm{K}}^{(\ell)} $ from DipB at r = 0.98R. The solid lines show the power spectra from early times (first 15 years) of the simulation, and the dashed lines the late times (last 15 years). Right panel: Temporal evolution of the dipolar contribution ( = 1) of the power spectra of the magnetic field E M $ \tilde{E}_{\mathrm{M}} $ from all the simulations. The values were normalized by E M ( 1 ) $ \tilde{E}_{\mathrm{M}}^{(1)} $ at the starting point of each simulation (at t0 = 85 years), for a better comparison.

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