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Fig. 2.

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Heat maps of ΔBz = Bz − Bz(t = 0) (first row), E (second row), Jz (third row), and (fourth row) for the HVM (left column, ), HVLF (central column, ), and iPIC (right column, ) simulations. These times are chosen by fixing the value of the reconnected magnetic flux. This value is in the middle of the super-exponential phase. The plot is zoomed-in around the main X point. The is the rms value of E in the shown region.

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