21 research outputs found

    Muon capture by 3He nuclei followed by proton and deuteron production

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    The paper describes an experiment aimed at studying muon capture by 3He{}^{3}\mathrm{He} nuclei in pure 3He{}^{3}\mathrm{He} and D2+3He\mathrm{D}_2 + {}^{3}\mathrm{He} mixtures at various densities. Energy distributions of protons and deuterons produced via Ό−+3He→p+n+n+ΜΌ\mu^-+{}^{3}\mathrm{He}\to p+n+n + \nu_{\mu } and Ό−+3He→d+n+ΜΌ\mu^-+{}^{3} \mathrm{He} \to d+n + \nu_{\mu} are measured for the energy intervals 10−4910 - 49 MeV and 13−3113 - 31 MeV, respectively. Muon capture rates, λcapp(ΔEp)\lambda_\mathrm{cap}^p (\Delta E_p) and λcapd(ΔEd)\lambda_\mathrm{cap}^d (\Delta E_d) are obtained using two different analysis methods. The least--squares methods gives λcapp=(36.7±1.2)s−1\lambda_\mathrm{cap}^p = (36.7\pm 1.2) {s}^{- 1}, λcapd=(21.3±1.6)s−1\lambda_\mathrm{cap}^d = (21.3 \pm 1.6) {s}^{- 1}. The Bayes theorem gives λcapp=(36.8±0.8)s−1\lambda_\mathrm{cap}^p = (36.8 \pm 0.8) {s}^{- 1}, λcapd=(21.9±0.6)s−1\lambda_\mathrm{cap}^d = (21.9 \pm 0.6) {s}^{- 1}. The experimental differential capture rates, dλcapp(Ep)/dEpd\lambda_\mathrm{cap}^p (E_p) / dE_p and dλcapd(Ed)/dEd d\lambda_\mathrm{cap}^d (E_d) / dE_d, are compared with theoretical calculations performed using the plane--wave impulse approximation (PWIA) with the realistic NN interaction Bonn B potential. Extrapolation to the full energy range yields total proton and deuteron capture rates in good agreement with former results.Comment: 17 pages, 13 figures, accepted for publication in PR

    Muon capture by ÂłHe nuclei followed by proton and deuteron production

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    The paper describes an experiment aimed at studying muon capture by He nuclei in pure ÂłHe and D₂+ÂłHe mixtures at various densities. Energy distributions of protons and deuterons produced via ”₋+ÂłHe-->p + n + n + Μ” and ”₋+ÂłHe-->d + n + Μ” are measured for the energy intervals 10–49 MeV and 13–31 MeV, respectively. Muon capture rates lambdacapp(ΔEp) and lambdacapd(ΔEd) are obtained using two different analysis methods. The least-squares methods give lambdacapp = (36.7±1.2) s–1, lambdacapd = (21.3±1.6) s–1. The Bayes theorem gives lambdacapp = (36.8±0.8) s–1, lambdacapd = (21.9±0.6) s–1. The experimental differential capture rates, dlambdacapp(Ep)/dEp and dlambdacapd(Ed)/dEd, are compared with theoretical calculations performed using the plane-wave impulse approximation with the realistic nearest-neighbor interaction Bonn B potential. Extrapolation to the full energy range yields total proton and deuteron capture rates in good agreement with former result

    Experimental study of ”-atomic and ”-molecular processes in pure helium and deuterium-helium mixtures

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    We present experimental results of ”-atomic and ”-molecular processes induced by negative muons in pure helium and helium-deuterium mixtures. The experiment was performed at the Paul Scherrer Institute (Switzerland). We measured relative intensities of muonic x-ray K series transitions in (”3,4He)* atoms in pure helium as well as in helium-deuterium mixtures. The d”³He radiative decay probabilities for two different helium densities in D2+³He mixture were also determined. Finally, the qHe1s probability for a d” atom formed in an excited state to reach the ground state was measured and compared with theoretical calculations using a simple cascade model
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