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Measurements of the C13(α,n)O16 cross section up to Eα=8 MeV

K. Brandenburg1,*, G. Hamad1, Z. Meisel1,†, C. R. Brune1, D. E. Carter1, R. J. deBoer2,‡, J. Derkin1, C. Feathers1, D. C. Ingram1 et al.

Y. Jones-Alberty1, B. Kenady1, T. N. Massey1, M. Saxena1, D. Soltesz1, S. K. Subedi1, A. V. Voinov1, J. Warren1, and M. Wiescher2

  • 1Institute of Nuclear and Particle Physics, Department of Physics and Astronomy, Ohio University, Athens, Ohio 45701, USA
  • 2The Joint Institute for Nuclear Astrophysics, Department of Physics and Astronomy, University of Notre Dame, Notre Dame, Indiana 46556 USA

  • *kb851615@ohio.edu
  • †meisel@ohio.edu
  • ‡rdeboer1@nd.edu

Phys. Rev. C 108, L061601 – Published 20 December, 2023

DOI: https://doi.org/10.1103/PhysRevC.108.L061601

Abstract

We present results from direct measurements of the total C13(α,n)O16 cross section over laboratory energies Eα=2.9–8.0 MeV, performed with the 3HeBF3 giant barrel neutron detector at the Edwards Accelerator Laboratory. The cross sections reported in this work are considerably lower than prior direct measurements for Eα>5 MeV, in agreement with prior corrections based on Hauser-Feshbach estimates. However, applying branching ratios based on Hauser-Feshbach estimates to our data would not reproduce existing direct measurements for partial decay channels. This indicates both the promise and limitations of Hauser-Feshbach for branching ratio estimates of (α,n) reactions on light nuclides. The C13(α,n) thick-target yields inferred from this work for Eα>6 MeV are significantly larger than those currently employed in estimates of dark matter and neutrino detector backgrounds.

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