# Concurrent application of ANC and THM to assess the $^{13}{\rm C}(\alpha,n)^{16}{\rm O}$ absolute cross section at astrophysical energies and possible consequences for neutron production in low-mass AGB stars

## TL;DR

This paper combines two indirect experimental methods to accurately determine the $^{13}{
m C}( ext{alpha},n)^{16}{
m O}$ reaction rate at astrophysical energies, reducing uncertainties in neutron production models in low-mass AGB stars.

## Contribution

It introduces a novel combined approach using ANC and THM to precisely measure the reaction rate relevant for stellar nucleosynthesis.

## Key findings

- Provided a highly accurate reaction rate for $^{13}{
m C}( ext{alpha},n)^{16}{
m O}$
- Reduced uncertainties in neutron production in low-mass AGB stars
- Showed limited impact on heavy element synthesis predictions

## Abstract

The $^{13}{\rm C}(\alpha,n)^{16}{\rm O}$ reaction is considered to be the main neutron source responsible for the production of heavy nuclides (from ${\rm Sr}$ to ${\rm Bi}$) through slow $n$-capture nucleosynthesis ($s$-process) at low temperatures during the asymptotic giant branch (AGB) phase of low mass stars ($\lesssim 3-4\;{\rm M}_{\odot}$, or LMSs). In recent years, several direct and indirect measurements have been carried out to determine the cross section at the energies of astrophysical interest (around $190\pm40\;{\rm keV}$). However, they yield inconsistent results causing a highly uncertain reaction rate and affecting the neutron release in LMSs. In this work we have combined two indirect approaches, the asymptotic normalization coefficient (or ANC) and the Trojan Horse Method (THM), to unambiguously determine the absolute value of the $^{13}{\rm C}(\alpha,n)^{16}{\rm O}$ astrophysical factor. Therefore, we have determined a very accurate reaction rate to be introduced into astrophysical models of $s$-process nucleosynthesis in LMSs. Calculations using such recommended rate have shown limited variations in the production of those neutron-rich nuclei (with $86\leq A\leq 209$) receiving contribution only by slow neutron captures.