Fig. 5
Maximum and total mass of the fragments (mmax and mtot, respectively)as a function of the clump gas temperature (T), the non-thermal velocity dispersion (σnth), and the ratiobetween σnth and the sound speed (cS), i.e. the Mach number. The typical uncertainties on the masses, mainly due to the mass opacity coefficient, can be up to a factor 2–3 (see Sect. 4.1).
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