Formation of the Neutron Donor 13C in AGB stars by overshoot and roation
F. Herwig1,2 and N. Langer3
Observations of heavy elements in red giant stars clearly show that low-mass AGB stars can provide a nucleosynthesis site of the s-process. Stellar evolution models produced over the last years indicate that radiative burning of 13C between succeeding thermal pulses in low-mass AGB star models may indeed provide the neutrons for the s-process. However, although it seems clear that some mixing between the proton-rich envelope and the carbon-rich core may lead to the production of 13C, the physical mechanism responsible for such mixing is not yet unambiguously identified. We present stellar model calculations which include mixing due to overshoot and rotation. Overshoot, with a time-dependent and exponentially decaying efficiency, leads to a partial mixture of protons and 12C during the third dredge-up (TDU), when the envelope convection zone reaches deep into the core. According to the depth-dependent ratio of protons and 12C, a small 13C pocket forms underneath a 14N-rich layer. Overshoot does not allow for any mixing after the envelope convection zone retreats at the end of the TDU after each pulse. Rotation introduces mixing driven by large angular velocity gradients which form at the envelope-core interface in AGB stars, in particular after a thermal pulse. This leads to partial mixing after a pulse, as in the case of overshoot. However, both mechanisms differ during the interpulse phase. Rotation continues to mix the region of the 13C-pocket. This does not only spread the 13C-pocket, but also the more massive 14N-rich layer, and finally leads to mixture of both layers. By the time when the temperature there has risen to about 9×107K and neutron production sets in, the 14N abundance exceeds the 13C abundance by a factor of 5...10. We analyze the role of 14N as a neutron poison by considering the recycling of neutron via 14N(n,p)14C and 12C(p, gamma)13N(beta+)13C qualitatively. We find that as long as X(14N) << X(12C), the s-process will still be possible to occur under radiative conditions.
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