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Fig. 6

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Cumulative distributions (a) and histograms (b) of sample model runs. An implantation factor of fimpl = 2 × 10−3 has been applied, after which the simulated distributions can be compared to the P48 population (black). In (b) the low number of bodies (and large Poisson error bars) illustrate why the fits tend to be rather insensitive to the specifics at the high-mass end of the distribution. Runs featuring small τs are associated with high σ due to the degeneracy between these quantities (see Table 3). Runs with small τs are disfavored, however, as pebble accretion operates too slowly.

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