- ... HBB
- Marigo (2003)
showed that variable molecular opacities may decrease the efficiency
of HBB - or even prevent it in some cases - especially in the more massive AGB stars.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... production
- We call attention to the fact that the MM02 yields for helium are currently the only ones to ensure a good agreement between chemical evolution models for the Milky Way (hereafter MW) and the solar helium abundance - see CMM03. This is essentially due to mass loss in massive stars. In the massive range, the yields computed by MM02 for He, C, N and O would be essentially unchanged
by explosive nucleosynthesis and can thus be considered robust calculations which take into account
important physics (i.e. rotation and mass loss - see Hirschi et al. 2004 for a detailed description of these models for massive stars).
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... CMM03
- For type Ia SNe we adopted the stellar yields of model W7 of Thielemann et al. (1993).
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... models
- Here we adopted their standard models and took their tables where the mass loss parameter varies with metallicity -
see CRM03 for details. vdHG97 also computed another set of models where less HBB was assumed.
We also computed a chemical evolution model where the latter stellar prescriptions were adopted.
In Fig. 2 this model would fall in between the two solid curves discussed here -
it is not shown to make the figure less crowded.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... points
- Romano & Matteucci (2003) have shown that by adopting the vdHG97 set of
stellar yields with less HBB it is possible to reproduce the trend of 12C/13C,
which decreases in time in the solar neighbourhood.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... C-rich
- Notice that Chieffi & Limongi (2002) do not include rotation in their computations.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... metallicity
- Some mechanism able to increase
14N at low metallicities is still needed in this case as models computed with WW95 stellar yields are not able to fit the new Spite et al. (2005) data for N/O, as shown by the thin solid curve in Fig. 2. WW95 also did not include
rotation in their calculations.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... metallicities
- Lower mass loss rates
lead to longer stellar lifetimes. As a consequence the star undergoes more dredge up episodes thus increasing the amount of C brought to the surface and later
ejected into the interstellar medium.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
- ... data
- Optical data suggest a flat N/O abundance gradient for the MW, whereas infrared data suggest a negative one (Simpson et al. 1995). Moreover, the recent data by Daflon & Cunha (2004) also show a gradient in N/O very similar
to the one obtained by our model once the MM02 stellar yields are adopted (compare asterisks and thick line shown in the middle panel of Fig. 5).
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.
.