Abstract

The neutron capture cross sections of light nuclei ($Al56$) are important for $s$-process scenarios since they act as neutron poisons. We report on measurements of the neutron capture cross sections of $^{41}\mathrm{K}$ and $^{45}\mathrm{Sc}$, which were performed at the Karlsruhe 3.7 MV Van de Graaff accelerator via the activation method in a quasistellar neutron spectrum corresponding to a thermal energy of $kT=25$ keV. Systematic effects were controlled by repeated irradiations, resulting in overall uncertainties of less than 3%. The measured spectrum-averaged data have been used to normalize the energy-dependent $(n,\ensuremath{\gamma})$ cross sections from the main data libraries JEFF-3.2, JENDL-4.0, and ENDF/B-VII.1, and a set of Maxwellian averaged cross sections was calculated for improving the $s$-process nucleosynthesis yields in AGB stars and in massive stars. At $kT=30$ keV, the new Maxwellian averaged cross sections of $^{41}\mathrm{K}$ and $^{45}\mathrm{Sc}$ are $19.2\ifmmode\pm\else\textpm\fi{}0.6$ mb and $61.3\ifmmode\pm\else\textpm\fi{}1.8$ mb, respectively. Both values are 20% lower than previously recommended. The effect of neutron poisons is discussed for nuclei with $Al56$ in general and for the investigated isotopes in particular.

Highlights

  • The light elements between 12C and 56Fe are important for the s-process scenario because they affect the neutron balance inside stars

  • The poisoning effect of the light isotopes between 12C and 56Fe can be illustrated at the example of thermally pulsing lowmass asymptotic giant branch (AGB) stars, where the s process takes place in two situations: between thermal instabilities via the 13C(α,n)16O reaction in the so-called 13C pocket at rather mild temperatures of about 90 MK and at the maximum extent of the thermal pulses via the 22Ne(α,n)25Mg reaction at temperatures near 250 MK [1,2]

  • In this paper we present the final (n,γ ) cross sections of 41K and 45Sc performed at the Karlsruhe 3.7 MV Van de Graaff accelerator

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Summary

Introduction

The light elements between 12C and 56Fe are important for the s-process scenario because they affect the neutron balance inside stars. Their neutron capture cross sections are small, these elements are much more abundant than those in the mass region above Fe. light elements constitute potential neutron poisons and may consume neutrons, which are not available for s-process nucleosynthesis. Light elements constitute potential neutron poisons and may consume neutrons, which are not available for s-process nucleosynthesis Important in this respect are neutron captures on the CNO elements and on the neon and magnesium isotopes, and other light isotopes up to iron contribute as well.

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