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The role of (some) nuclear reaction rates in the evolution of the stars of low, intermediate and high mass. Alessandro Chieffi (Istituto di Astrofisica Spaziale e Fisica Cosmica & INAF) Email: achieffi@rm.iasf.cnr.it. 25 M O. 5 M O. 1 M O. REMEMBER that:
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The role of (some) nuclear reaction rates in the evolution of the stars of low, intermediate and high mass Alessandro Chieffi (Istituto di Astrofisica Spaziale e Fisica Cosmica & INAF) Email: achieffi@rm.iasf.cnr.it
25 MO 5 MO 1 MO
REMEMBER that: The interplay between the evolution of a star and the nuclear processes occurs through the RATES and NOT the cross sections: Rlk => Xl x Xk x screening x <sv>lk
25 MO Dt(H-burn)= - 0.3% M(He) => 8.3 to 8.6 MO CNO cycle <sv>3a x 10 is NOT appreciable 14N(p,g)15O x 10 5 MO CNO cycle M(He) => 0.91 to 0.97 MO Dt(H-burn)= - 4% 1 MO PP chain p(p,e+n)d Dt(H-burn)= - 3%
HB RGB TO MS
Z=10-4 Y=0.23 Solid => reference Dashed => (14N(p,g)15O) / 2 10 Gyr 13 Gyr
M=0.8 MO Y=0.23 Z=10-4 Red – reference Blue – 14N(p,g)15O / 2 • MHe = 1% • Mbol(tip) = 0.055 Mag -0.04 Mag => - 0.6 Gyr
AGB phase 0.7 < M / MO < 7 He burning shell R(Hshell) ~10-5 Rstar CO core He (+C) intershell Neutron production s process nucleosynthesis H burning shell H-rich mantle
Convective envelope H shell M(MO) He shell t(yr)
Convective envelope H shell M(MO) He conv. shell He shell t(yr)
-1 8.5 7.5 Base conv. env. H burn. shell He burn. shell Log(Surf. C abund.) Log(Tmax He shell) Log(T base conv. Env.) -3 8.1 6.5
M=3 MO Z=0.02 Y=0.284 Network: H to Si (full) + Neutron captures on: Fe Kr84 – Rb – Sr – Y – Zr92 Xe132 – Cs – Ba – La – Ce – Pr – Nd144 Hg202 – Tl – Pb – Bi209 92 nuclei
Log10(PF) Element
Log10(PF) Stable Isotopes
M=3 MO - Z=0.02 Reference 3a / 2 3a x 2 14Npg / 2
SURFACE CARBON ABUNDANCE Reference 3a / 2 3a x 2 14Npg / 2
Roadmap... 1) WR stars: evolution & explosive nucleosynthesis 120 35 2) Intermediate Mass Stars: elemental yields