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Fig. 3

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Radial distribution of the electron density (A), the equipartition magnetic field (B), and the product of the two with (D) and without (C) redshift dilution, for Mclust = 1015 M and ɀmax = 4. Each value at a given radius is the skew-normal median of the values of all Ntree = 103 MTs. We can see that the ne profiles decrease more than that of Bequ. Without redshift dilution, we would expect ne to play a major role in the RM decay. However, because of the (1 + ɀ)−2 factor, RM curves evolve very little over time.

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