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
Summary
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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