“…We will not review the physics of these stellar tracks here but we just mention that over the years, these models were calculated including semi-convection in massive stars (e.g., Chiosi & Summa 1970), ballistic-convective overshooting from the core (Bressan, Chiosi & Bertelli 1981), overshooting from the the bottom of the convective envelope (Alongi et al 1991), turbulent diffusion from the convective core and convective shells Deng, Bressan & Chiosi (1996a,b); Salasnich, Bressan & Chiosi (1999), plus several additional improvements and revisions (Alongi et al 1993; Fagotto et al 1994b;Bertelli et al 1994;Fagotto et al 1994a,a;Bertelli & Nasi 2001;Bertelli et al 2003Bertelli et al , 2008Bertelli et al , 2009. The stellar models in use are those by Bertelli et al (2008Bertelli et al ( , 2009), which cover a wide grid of helium Y , metallicity Z, and enrichment ratio ∆Y /∆Z. The associated isochrones include the effect of mass loss by stellar wind and the thermally pulsing AGB phase according to the models calculated by Marigo & Girardi (2007).…”