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Table 1.

Summary of our population synthesis runs, best match shaded with colour.

SFR SF for QHe II L1550 Source of C IV emission QH I I(4686)
[M yr−1] [Myr] [ph. s−1] [erg s−1] [ph. s−1] /I(Hβ)
fiducial 0.1 3 1.80⋅1050 3.71⋅1037 one/two WOs of > 90 M 7.02⋅1052 0.004
NE: 0.69⋅1050 NE: 6.21⋅1052
CHE: 1.11⋅1050 CHE: 0.81⋅1052

SF-10 0.03 10 1.96⋅1050 3.43⋅1037 six WOs of 40 M 3.15⋅1052 0.011
NE: 0.14⋅1050 & one of 80 M NE: 2.62⋅1052
CHE: 1.82⋅1050 CHE: 0.53⋅1052

SF-15 0.02 15 2.19⋅1050 2.83⋅1037 ∼twenty WOs of 25 M 2.23⋅1052 0.017
NE: 0.09⋅1050 & two of 50 M NE: 1.75⋅1052
CHE: 2.10⋅1050 CHE: 0.48⋅1052

SF-15-80 0.02 15 1.94⋅1050 2.15⋅1037 seventeen WOs of 20 M 1.96⋅1052 0.017
NE: 0.06⋅1050 & ∼four of 40 M NE: 1.53⋅1052
CHE: 1.88⋅1050 CHE: 0.43⋅1052

SF-15-40 0.02 15 1.31⋅1050 0.91⋅1037 seventeen WOs of 20 M 1.38⋅1052 0.016
NE: 0.01⋅1050 & ∼three of 30 M NE: 1.07⋅1052
CHE: 1.30⋅1050 CHE: 0.31⋅1052

Notes. All runs assumed a Salpeter IMF with Mtop ≤ 150 M (see label) and 10% of stars rotating fast enough for chemically homogeneous evolution. The total size of the region formed is 3⋅105 M in all cases. For reference, the observed values are Q He II obs $ ^{\mathrm{obs}}_{{\mathrm{He}{\small { {\text{ II}}}}}} $ = 1.33⋅1050 photons s−1 and L 1550 obs $ ^{\mathrm{obs}}_{1550} $ = 2.2–5.5⋅1037 erg s−1. Our results from most runs are able to account for these, regardless of the various assumptions about the star-formation history and thus, the stellar content. The fiducial case mimics the scenario in Paper I (details are given in Sect. 2.3), while the others relax the SFR, lower the Mtop, and lengthen the age of the population, meaning later phases of lower-mass models are captured. This is why the source of the stellar C IV emission gets less and less extreme: after the third case, no very massive star (VMS) is needed at all. As for the observed hardness, i.e. the relative intensity of I(4686)/I(H[[INLINE286]]) = A⋅Q(He II)/Q(H I), it should be between 0.02−0.04 observationally, which renders our third population most consistent with measurements (including the C IV line luminosity, which becomes lower with smaller Mtop) and thus most favoured, as explained in Sect. 3.2 (also see Fig. 7).

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