As Fig. 6, but with v sin i values for the synthetic population calculated by applying our new angular momentum loss recipe to the models of Brott et al. (2011), as discussed in Appendix A. The simulated distribution reaches beyond the y-axis boundary in four panels. For the 60–100 M_⊙ mass bin, the third quarter reaches to 0.08 and the fourth quarter reaches to 0.17. For the 40–60 M_⊙ mass bin, the fourth quarter reaches to 0.12. For the 30–40 M_⊙ mass bin the fourth quarter reaches to 0.05.