Table 1
Properties of the 13C-pocket models.
| Y p | 13C burninga | MPMZ(M⊙) |  (M⊙) |
Artificial MTDU(10-3M⊙) | ||||
|
|
||||||||
| J004441 | J050632 | J052043 | J053250 | |||||
| pocket_case1 | standardb | radiative | 1.8 × 10-3 | 1.35 × 10-4 | 45.3 | 1.05 | 3.13 | 4.16 |
| pocket_case2 | standardb | convective | 1.0 × 10-3 | 7.50 × 10-5 | 3.77 | 0.18 | 0.51 | 0.67 |
| pocket_case3 | 0.70 × 10-4 | radiative | 1.8 × 10-3 | 1.26 × 10-7 | 87 | 1.33 | 4.03 | 5.40 |
| pocket_case4 | 1.05 × 10-4 | radiative | 1.8 × 10-3 | 1.89 × 10-7 | 6.04 | 0.27 | 0.78 | 1.02 |
| pocket_case5 | 1.05 × 10-4 | radiative | 3.6 × 10-3 | 3.78 × 10-7 | 2.76 | 0.14 | 0.39 | 0.50 |
Notes. MTDU is given for the models that include only one 13C pocket.
Refers to the usual case where all the 13C burns in radiative conditions during the interpulse period or the case where we forced the 13C to burn in convective conditions while it is ingested in the following TP.
Refers to a proton abundance Yp that decreases exponentially with the mass depth from the envelope value to 10-4 at a mass depth MPMZ below the base of the envelope (Fig. 2).
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