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Fig. 3.

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Structure of the reference shock with Ms = 3, β = 20, and θBn = 75° (run A4) at different times Ωcit = 10 (panels a*), Ωcit = 30 (panels b*), and Ωcit = 55 (panels c*). From top to bottom, shown are the maps of the normalized ion density, Ni/N0i (panels *1), and the normalized magnetic field fluctuations (see Eqs. (8)–(10)), δBx (panels *2), δBy (panels *3), and δBz (panels *4). The scaling of all distributions is logarithmic and for the magnetic fields it is sign-preserving, and, e.g., for δBz it is: sgn(δBz)⋅{2 + log[max(|δBz|/B0, 10−2)]}. The level of “0” on the color scale hence corresponds to |δB|/B0 ≤ 10−2 (see, e.g., Kobzar et al. 2021).

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