Abstract

Reaction rates of the $$^{11}$$ B(p, $$\alpha$$ ) $$\alpha \alpha$$ process have been evaluated on the basis of a data set spanning incident proton energies $$E_p$$ from 0.15 to 3.8 MeV. A previously published analysis (Spraker et al. in J Fusion Energy 31(4):357, 2012) of these data provided the number of outgoing $$\alpha$$ -particles in a restricted range of the detected $$\alpha$$ -energy spectrum, making it unsuitable for the evaluation of the reaction rates. The present work takes advantage of a calculation of the $$\alpha$$ -energy spectrum based on a sequential model of the reaction and the assumption that the primary $$\alpha$$ -particles are emitted with $$\ell =3$$ . A full description of this ansatz, which has been shown to reproduce the essential features of the observed $$\alpha$$ -energy spectra, can be found in Stave et al. (Phys Lett B 696:26, 2011). The accuracy of these calculated spectra has made it possible to reliably extrapolate the new data to zero-energy $$\alpha$$ -particles. In the ensuing calculation of the cross section, the total measured $$\alpha$$ -yield is then divided by a fixed factor of three at all incident proton energies. In addition, this technique has enabled a treatment of the $$\alpha _0$$ channel where the 12C nuclei decay to the ground state of 8Be via emission of an $$\alpha$$ -particle. This channel contributes at incident proton energies above 2 MeV. The new cross section data have then been used to evaluate the $$^{11}$$ B(p, $$\alpha$$ ) $$\alpha \alpha$$ reaction rates. The new evaluation is $$\sim$$ 10–15 % higher than the currently accepted result (Angulo et al. in Nucl Phys A 656(1):3, 1999) at temperatures between 200 and 600 keV (2–7 $$\times$$ 10 $$^9$$ K). The inclusion of a narrow, low-lying resonance at $$E_p=0.162$$ MeV in the evaluation is found to have a minimal effect on the reaction rate above 100 keV (1.2 $$\times$$ 10 $$^9$$ K), and a higher-lying state at $$E_p=3.75$$ MeV is shown to enhance the reaction rates by only $$\sim$$ 15 % above 400 keV (4.6 $$\times$$ 10 $$^9$$ K).

Highlights

  • The 11B(p,a)aa reaction at incident proton energies Ep\4 MeV has been studied since the 1930s [4–8]

  • In the ensuing calculation of the cross section, the total measured a-yield is divided by a fixed factor of three at all incident proton energies. This technique has enabled a treatment of the a0 channel where the 12C nuclei decay to the ground state of 8Be via emission of an aparticle

  • Based on cross section data collected previously at the Triangle Universities Nuclear Laboratory (TUNL) [1] and a model of the reaction mechanism developed to account for the observed a-energy spectra [2], the reaction can be described via its behavior at resonances at Ep 1⁄4 0:675 and Ep 1⁄4 2:64 MeV

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Summary

Introduction

The 11B(p,a)aa reaction at incident proton energies Ep\4 MeV has been studied since the 1930s [4–8]. Abstract Reaction rates of the 11B(p,a)aa process have been evaluated on the basis of a data set spanning incident proton energies Ep from 0.15 to 3.8 MeV.

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