We have measured π±p and pp elastic differential cross sections in the range |cosθc.m.|<0.35 for incident momenta from 2 to 9.7 GeV/c for π−p and pp and from 2 to 6.3 GeV/c for π+p. We find that the fixed-c.m.-angle πp differential cross sections cannot be described as simple functions of s. The data are compared to the energy and angular dependence predicted by the constituent model of Gunion, Brodsky, and Blankenbecler.
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An optical spark chamber and neutron time-of-flight spectrometer experiment studied the reaction π−p→π+π−n at incident pion momentum of 4.5 GeVc in the mass region of the f0 meson. Analysis of the data shows no evidence for anomalous structure in the f0 mass spectrum. The two-pion differential cross section in the f0 region is consistent with Wolf's one-pion-exchange model for momentum transfers (squared) −t≲0.7 (GeVc))2. The differential cross section is larger than that predicted at high momentum transfer, and may be attributed to natural-parity-exchange contributions as evidenced in the f0 decay distribution.
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DIPION PRODUCTION CROSS SECTION NORMALIZED AT LOW -T TO A WOLF-MODEL F CROSS SECTION OF 400 MUB.
An experiment using optical spark chambers and a neutron time-of-flight hodoscope has been performed at the Argonne National Laboratory on the reaction π−p→ω0n. The differential cross section and the experimentally accessible density-matrix elements were determined in the momentum transfer interval 0.05≤|t|≤1.0 (GeV/c)2 at each of three incident pion momenta 3.65, 4.50, and 5.50 GeV/c. Our results show the following general features: (1) a dip in the forward differential cross section for |t|≤0.2 (GeV/c)2, (2) a slope at larger momentum transfers which increases as the incident pion momentum increases, and (3) no dips in either dσdt or ρ11+ρ1−1, the natural-parity exchange combination, at |t|=0.6 (GeV/c)2.
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