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|Tz|=32Δ(1238) systems are studied from the standpoint of direct production utilizing experimental data on the reactions pp→pπ+n, pp→pπ+π−p, pp→pπ+π−π0p, and pp→pπ+π−π+n. Resonance-production total and differential cross sections are presented, in addition to the decay density-matrix elements. It is demonstrated that the experimentally defined Δ(1238) systems are not characterized solely by spin-parity 32+, and that corresponding elements of the density matrices of both pπ+ and π−n cases generally behave in a similar manner with increasing c.m. angle. Additional detailed studies of the t-channel moments are presented for peripherally produced πN systems as a function of both c.m. angle and πN invariant mass. Dynamical differences are observed between the pπ+ and nπ− moments for the very peripheral data. One-pion-exchange-model predictions are compared with the peripheral pπ+ moments and with several invariant-mass distributions from the pp→pπ+π−p data. Complications arising from the presence of two pπ+ combinations in the four- and five-body final-state data are discussed.
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We have studied the 2 π 0 final states in the reaction π + d → π 0 π 0 p(p) at 2.15 GeV/ c in a 2 million picture exposure of the PPA rapid cycling deuterium bubble chamber. Two tantalum plates were added to the bubble chamber to convert γ rays which were kinematically constrained to a 2 π 0 hypothesis. The 2 π 0 mass spectrum is observed to saturate s-wave unitarity in the ππ mass region between 0.6 and 0.9 GeV/ c 2 , clearly favoring the ‘up-down’ or broad resonance solution for s-wave, I = 0, ππ scattering.
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Measurements have been made of the total charge-exchange cross section π − p to π 0 n over the laboratory kinetic energy range 90 to 290 MeV. The data have an absolute accuracy of typically 1%, and have here been used to determine the pion-nucleon P 13 phase shift.
QUADRATIC INTERPOLATION.
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