Fig. 11.

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Hertzsprung-Russell diagram tracks of our 30 and 60 M⊙ model subjected to different mass-loss rates which are kept fixed during the core-He-burning RSG phase. No mass loss is applied till log(Teff)=3.7 below which the models are subjected to a constant mass-loss rate specified in the legend. The luminosity of RSGs during core-He burning is primarily determined by the He core mass, which remains largely insensitive to the mass-loss rate.
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