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Coincidence measurements of (<i>p</i>,<i>n</i>) reactions at 1.5 GeV/<i>c</i>on C and H in the Δ excitation region

J. ChibaNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanT. KobayashiNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanT. NagaeNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanI. AraiNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanNorihisa KatôNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanH KitayamaNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanA. ManabeNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanM. TanakaNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanK. TomizawaNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanD. BeattyNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanG. EdwardsNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanC. GlashausserNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanG. KumbartzkiNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanR. D. RansomeNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, JapanF. T. BakerNational Laboratory for High Energy Physics (KEK), Oho, Tsukuba-shi, Ibaraki 305, Japan
1991en
ABI

Annotatsiya

Coincidence measurements of (p,n) reactions at 1.5 GeV/c in the \ensuremath{\Delta} excitation region have been carried out for the first time. The location of the \ensuremath{\Delta} peak in the neutron spectrum is found to be dependent on the coincident particles. The peak in coincidence with p${\mathrm{\ensuremath{\pi}}}^{+}$ is shifted to lower momenta compared to the free case, in contrast to the inclusive spectrum and the coincidence with other particles where it is shifted to higher momenta. The p${\mathrm{\ensuremath{\pi}}}^{+}$ invariant-mass distribution for C is significantly lower and broader than that for H. The coincidence data set stringent constraints on theoretical models introduced to interpret the peak shift in inclusive spectra.

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