Abstract

Angular distributions of the differential cross sections and analyzing powers have been measured for the $^{3}\mathrm{He}$(p\ensuremath{\rightarrow},${\mathrm{\ensuremath{\pi}}}^{+}$) $^{4}\mathrm{He}$ and $^{4}\mathrm{He}$(p\ensuremath{\rightarrow},${\mathrm{\ensuremath{\pi}}}^{+}$${)}^{5}$He reactions at proton bombarding energies between 240 and 507 MeV. These new results provide a comprehensive set of data spanning the region of the ${\mathrm{\ensuremath{\Delta}}}_{1232}$ resonance and are compared with a phenomenological model that incorporates the amplitudes for the pp\ensuremath{\rightarrow}d${\mathrm{\ensuremath{\pi}}}^{+}$ reaction, and with calculations from a microscopic (p,${\mathrm{\ensuremath{\pi}}}^{+}$) model. A $^{5}\mathrm{He}$ final state interaction calculation based upon the low energy n+\ensuremath{\alpha} elastic phase shifts indicates that the $^{4}\mathrm{He}$(p,${\mathrm{\ensuremath{\pi}}}^{+}$${)}^{5}$He spectra are nearly independent of pion angle and proton energy. Comparisons made with the time reversed charge symmetric reaction $^{3}\mathrm{H}$(n,${\mathrm{\ensuremath{\pi}}}^{\mathrm{\ensuremath{-}}}$${)}^{4}$He reaction indicate substantial Coulomb effects are still present at 300 MeV.

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