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| Nucleosynthesis in Fallback Ejecta |
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... Fallback
... Ti44 + Ni56
... He shell flash
... SNIa ignition
... Flames with 22Ne
... P-rich NSE
... Verification
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J.D. Maldonado
F.X.Timmes, my vitae
Brad Meyer's PRL", "The r-Process without Excess Neutrons", is relevant.
Without mincing words, we propose a new origin site and a new mechanism for the r-process.
Total abundance patterns
Some rapid neutron signatures jpg or pdf |
95% r-process isotopes |
Thermodynamic evolutions
Temperature, 5e9 cm scale, 23MB |
Temperature, 1e9 cm scale, 53MB |
Temperature, 1e8 cm scale, 30MB |
Density, 5e9 cm scale, 24MB |
Density, 1e9 cm scale, 51MB |
Density, 1e8 cm scale, 31MB |
Isotope evolutions
4He, 1e9 cm scale, 18MB |
4He, 1e8 cm scale, 22MB |
4He, 1e7 cm scale, 22MB |
56Ni, 1e9 cm scale, 43MB |
56Ni, 1e8 cm scale, 33MB |
56Ni, 1e7 cm scale, 15MB |
Particle 3318 evolution
Particle 3318, Ye=0.5, 38MB |
Particle 3318, Ye=0.5, thermodynamics |
Particle 3318 collage jpg or pdf In column format: pdf In its 4 parts: part01, part02, part03, part04 |
Particle 3318, The Meyer Ratio - ala figure 2 of Brad's paper - jpg or pdf |
Particle 0006 sensitivities
Particle 6 Ye collage jpg or pdf In its 3 parts: part01, part02, part03, |
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Particle 6 Ye=0.5 |
Particle 6 Ye=0.500 |
Particle 6 Ye=0.500 |
Particle 6 Ye=0.501 |
Particle 6 Ye=0.501 |
Particle 6 Ye=0.505 |
Particle 6 Ye=0.505 |
Particle 6 Ye=0.510 |
Particle 6 Ye=0.510 |
Particle 6 Ye=0.520 |
Particle 6 Ye=0.520 |
Particle 6 Ye=0.499 |
Particle 6 Ye=0.499 |
Particle 6 Ye=0.495 |
Particle 6 Ye=0.495 |
Particle 6 Ye=0.490 |
Particle 6 Ye=0.490 |
Particle 6 Ye=0.480 |
Particle 6 Ye=0.490 |
aion = 195 particles
Evolution of the top 20 particles that make the 3rd peak: a195_top20_evolutions.tar.bz2 (116 MB)
top 20 a=195 peak particles |