Issue |
EPJ Web Conf.
Volume 275, 2023
11ᵗʰ European Summer School on Experimental Nuclear Astrophysics
|
|
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Article Number | 02014 | |
Number of page(s) | 4 | |
Section | Session 2: Contribution by Young Researchers | |
DOI | https://doi.org/10.1051/epjconf/202327502014 | |
Published online | 03 February 2023 |
https://doi.org/10.1051/epjconf/202327502014
13C(α,n)16O: The Source of Neutrons for the s-process main component
1 Manipal Centre for Natural Sciences, Manipal Academy of Higher Education, Manipal - 576104, India
2 Physics Department, Faculty of Science, M. S. University of Baroda, Vadodara - 390002, India
3 Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, Catania - 95123, Italy
4 Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai - 400085, India
5 Manipal Institute of Technology, Manipal Academy of Higher Education, Manipal - 576104, India
* e-mail: pareshkumar.p@manipal.edu
Published online: 3 February 2023
The 13C(α, n)16O reaction operates in the He intershell of low-mass(M < 4 M⊙) AGB stars and it is the neutron source that allows the creation of the main component of the s-process elements. The reaction rate is then required to be well known in the energy range of astrophysical interest. Therefore, the 13C(α, n)16O reaction rate has been calculated in stellar like conditions using a nuclear-model based computer code TALYS. The results have been compared with available literature data and found to be in good agreement with experimental data and, evaluated data NACRE II as well.
© The Authors, published by EDP Sciences, 2023
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