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Fig. B.2.

image

Comparison of the prestellar CMF observed in Orion B (black triangular data points and histogram from Könyves et al. 2019; see also Fig. 3) with the global prestellar CMFs expected in the toy model of Sect. 3, under three assumptions about the shape of the CMF generated by a single filament of line mass Mline: (i) lognormal fMline(m) distribution (Eq. (2)) with (fiducial case, black curve); (ii) lognormal fMline(m) distribution (Eq. (2)) with fixed σMline = 0.2 independent of Mline (blue curve); and (iii) broken power law, fMline(m)∝m6 for m <  MBE, th, fMline(m) = constant for MBE, th ≤ m <  MBE, eff, fMline(m)∝m−4 for m >  MBE, eff (red curve). For reference, the black dotted line displays the Salpeter-like power-law FLMF, dN/dlog , observed in the supercritical line mass regime (see Fig. 1), and the black dash-dotted line shows the typical mass distribution of CO clumps (Kramer et al. 1998).

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