We present a nucleosynthesis calculation of a 25 M-circle dot star of solar composition that includes all relevant isotopes up to polonium. We follow the stellar evolution from hydrogen burning till iron core collapse and simulate the explosion using a 'piston' approach. We discuss the influence of two key nuclear reaction rates, C-12(alpha, gamma)O-16 and Ne-22(alpha, n)Mg-25, on stellar evolution and nucleosynthesis. The former significantly influences the resulting core sizes (iron, silicon, oxygen) and the overall presupernova structure of the star. It thus has significant consequences for the supernova explosion itself and the compact remnant formed. The later rate considerably affects the s-process in massive stars and we demonstrate ...
The s-process in massive stars produces the weak component of the s-process (nuclei up to A ∼ 90), i...
The astrophysical p process, which is responsible for the origin of the proton rich stable nuclei he...
The s-process in massive stars produces the weak component of the s-process (nuclei up to A ~ 90), i...
We present the first calculations to follow the evolution of all stable nuclei and their radioactive...
We present the first calculations to follow the evolution of all stable nuclei and their radioactive...
We have performed the first calculations to follow the evolution of all stable nuclei and their radi...
Preliminary results of a new set of stellar evolution and nucleosynthesis calculations for massive s...
We present the first calculations to follow the evolution of all stable isotopes and their abundant ...
Properties of atomic nuclei important for the prediction of astrophysical reaction rates are reviewe...
We present a comprehensive study of s-process nucleosynthesis in 15, 20, 25, and 30 $\msun$ stellar ...
Hans Bethe contributed in many ways to our understanding of the supernovae that happen in massive st...
This overview discusses issues relevant to modeling nucleosynthesis in type II supernovae and implic...
The nucleosynthetic yield of isotopes lighter than A = 66 (zinc) is determined for a grid of stellar...
We present a new set of presupernova evolutions and explosive yields of massive stars of initial sol...
We explore the sensitivity of the nucleosynthesis of intermediate-mass elements (28 less than or equ...
The s-process in massive stars produces the weak component of the s-process (nuclei up to A ∼ 90), i...
The astrophysical p process, which is responsible for the origin of the proton rich stable nuclei he...
The s-process in massive stars produces the weak component of the s-process (nuclei up to A ~ 90), i...
We present the first calculations to follow the evolution of all stable nuclei and their radioactive...
We present the first calculations to follow the evolution of all stable nuclei and their radioactive...
We have performed the first calculations to follow the evolution of all stable nuclei and their radi...
Preliminary results of a new set of stellar evolution and nucleosynthesis calculations for massive s...
We present the first calculations to follow the evolution of all stable isotopes and their abundant ...
Properties of atomic nuclei important for the prediction of astrophysical reaction rates are reviewe...
We present a comprehensive study of s-process nucleosynthesis in 15, 20, 25, and 30 $\msun$ stellar ...
Hans Bethe contributed in many ways to our understanding of the supernovae that happen in massive st...
This overview discusses issues relevant to modeling nucleosynthesis in type II supernovae and implic...
The nucleosynthetic yield of isotopes lighter than A = 66 (zinc) is determined for a grid of stellar...
We present a new set of presupernova evolutions and explosive yields of massive stars of initial sol...
We explore the sensitivity of the nucleosynthesis of intermediate-mass elements (28 less than or equ...
The s-process in massive stars produces the weak component of the s-process (nuclei up to A ∼ 90), i...
The astrophysical p process, which is responsible for the origin of the proton rich stable nuclei he...
The s-process in massive stars produces the weak component of the s-process (nuclei up to A ~ 90), i...