RADIATIVE C-13 BURNING IN ASYMPTOTIC GIANT BRANCH STARS AND S-PROCESSING

被引:271
作者
STRANIERO, O
GALLINO, R
BUSSO, M
CHIEFFI, A
RAITERI, CM
LIMONGI, M
SALARIS, M
机构
[1] UNIV TURIN,IST FIS GEN,I-10125 TURIN,ITALY
[2] OSSERV ASTRON TORINO,I-10025 PINO TORINESE,ITALY
[3] CNR,IST ASTROFIS SPAZIALE,I-00044 FRASCATI,ITALY
[4] OSSERV ASTRON ROMA,I-00040 MONTE PORZIO CATO,ITALY
[5] CNR,IST ASTROFIS SPAZIALE,ROME,ITALY
[6] UNIV ROME,IST ASTRON,ROME,ITALY
关键词
NUCLEAR REACTIONS; NUCLEOSYNTHESIS; ABUNDANCES; STARS; AGB AND POST-AGB; EVOLUTION;
D O I
10.1086/187767
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present new evolutionary calculations for a 3 M. star of Population I starting from the zero-age main sequence and followed up to the 25th thermal pulse of the asymptotic giant branch. The third dredge-up is found to occur in a self-consistent way from the 14th pulse on. We show that any amount of C-13 possibly synthesized at the H/He interface during the interpulse period is completely burnt through (alpha, n) reactions before the next pulse develops. As a consequence, s-elements are produced in a radiative environment, at a neutron density of at most a few 10(7) n cm(-3). They are then engulfed and diluted into the next convective pulse, where a second (minor) neutron burst occurs, driven by the Ne-22(alpha, n)Mg-25 reaction marginally activated near the end of the He-shell instability. Despite the differences of the present model with respect to past calculations, we predict s-process distributions very close to those computed by allowing C-13 to burn in convective pulses: C-13 burning and the ensuing s-processing are confirmed to account for the main observational and experimental constraints. The reasons for this are briefly discussed. Since no C-13 survives the interpulse phase, we conclude that no modifications of the pulse shape due to the energy feedback from the C-13(alpha, n)O-16 reaction occur.
引用
收藏
页码:L85 / L87
页数:3
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