We present the 26 Al and 60 Fe yields produced by a generation of solar metallicity stars ranging in mass between 11 and 120 M ☉ . We discuss the production sites of these γ-ray emitters and quantify the relative contributions of the various components. We provide the contributions of the wind, the C convective shell, and the explosive Ne/C burning to the total 26 Al yield together with the contributions of the He convective shell, the C convective shell, and the explosive Ne/C burning to the 60 Fe yield. We conclude that, at variance with current beliefs, 26 Al is mainly produced by the explosive C/Ne burning over most of the mass interval analyzed here, while 60 Fe is mainly produced by the C convective shell and the He convective shell. By means of these yields we try to reproduce two quite strong observational constraints related to the abundances of these nuclei in the interstellar medium, i.e., the number of γ 1.8 photons per Lyman continuum photon, R GxL , and the 60 Fe/ 26 Al γ-ray line flux ratio. R GxL is found to be roughly constant along the Galactic plane (and of the order of 1.25 × 10 -11 ), while the 60 Fe/ 26 Al ratio has been recently measured by both RHESSI (0.17 ± 0.05) and SPI ( INTEGRAL ) (0.11 ± 0.03). We can quite successfully fit simultaneously both ratios for a quite large range of exponents of the power-law initial mass function. We also address the fit to γ 2 Velorum, and we find that a quite large range of initial masses, at least from 40 to 60 M ☉ , do eject an amount of 26 Al (through the wind) compatible with the current upper limit quoted for this W-R star: such a result removes a long-standing discrepancy between the models and the observational data.
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Limongi et al. (2006) studied this question.
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