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A new way to unravel the <sup>12</sup>C(α,γ)<sup>16</sup>O cross section components using neural networks

ORAL

Abstract

The 12C(α,γ)16O reaction rate plays a crucial role in determining the 12C to 16O abundance ratio in various stellar nucleosynthesis scenarios. Measuring the cross section for this reaction at stellar energies is challenging because of its extremely small size, estimated to be about 10−17 b at Ec.m. = 300 keV. To overcome this limitation, R-matrix calculations are used to extrapolate the data to lower energies. These calculations rely on a comprehensive understanding of each contribution to the cross section. The dominant contributions to the cross section at stellar energies arise from the electric dipole (E1) and electric quadrupole (E2) transitions to the ground state of 16O, accompanied by a non-negligible cascade contribution. Traditionally, these contributions have been separated using the γ-ray angular distribution. In this work, we propose a novel technique that uses the energy distribution of the 16O recoils at the focal plane. The analysis utilizes a neural network trained on a detailed Monte Carlo simulation of the transport of the recoils through the recoils mass separator ERNA. This approach will enable us to simultaneously determine all three contributions achieving systematic uncertainties better than 10% for the ground state contributions and better than 14% for the cascade contribution in the energy region from Ec.m. = 1 to 2.2 MeV. By employing this new technique, we aim to improve the accuracy in determining the cross section of the 12C(α,γ)16O reaction at astrophysical energies.

Publication: The results will be submitted to The European Physical Journal A.

Presenters

  • Jeremias Garcia-Duarte

    Lawrence Livermore National Laboratory Chapters

Authors

  • Jeremias Garcia-Duarte

    Lawrence Livermore National Laboratory Chapters

  • Antonino Di Leva

    Department of Physics, University of Naples "Federico II", 80126 Napoli, Italy

  • Raffaele Buompane

    Department of Mathematics and Physics, University of Campania "Luigi Vanvitelli", 81100 Caserta, Italy

  • Alba Formicola

    5National Institute for Nuclear Physics (INFN) - Laboratori Nazionali del Gran Sasso, 67100 L'Aquila, Italy

  • Jason T Harke

    Lawrence Livermore National Laboratory, Livermore, California 94550, USA

  • Davide Rapagnani

    Department of Physics, University of Naples "Federico II", 80126 Napoli, Italy

  • Claudio Santonastaso

    Department of Mathematics and Physics, University of Campania "Luigi Vanvitelli", 81100 Caserta, Italy

  • Lucio Gialanella

    Department of Mathematics and Physics, University of Campania "Luigi Vanvitelli", 81100 Caserta, Italy