Turbulent dynamo action and its effects on the mixing at the convective boundary of an idealized oxygen-burning shell

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Fig. 10.

Vertical profiles of the root-mean-square relative pseudo-entropy fluctuation in the MHD (light blue) and purely hydrodynamic simulations (vermilion), averaged over t ∈ (15τ_conv, 25τ_conv). The upper convective boundary is, on average, at the position of the peaks visible at y = (2.3 − 2.4) L_ref.

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