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Fig. 4


Time and z dependence of (top) and (middle) for a dynamo simulation with the reference solution parameters. We note that has been normalised by the product of urms (0.035) and the corresponding rms magnetic field, brms (0.036), both of which have been time-averaged over the given time period. Bottom: results of temporally smoothing , using a sliding (boxcar) average with a width of approximately 50 convective turnover times.

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