1965
DOI: 10.1103/physrev.137.b962
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Experimental Study of Particle Production at Small Angles in Nucleon-Nucleon Collisions at 19 and 23 GeV/c

Abstract: Differential cross sections are presented for the production of pions, kaons, protons, and antiprotons at the angles 0° and 5.7°, produced in proton collisions with H2, Be, and Pb targets at primary momenta of 18.8 and 23.1 GeV/c, and in some cases at 8.65 and 11.8 GeV/c. The data are discussed with special reference to the role of isobar excitation in the production of secondary particles. All qualitative features of the experimental data are shown to be consistent with a dominant role of isobar decay in the … Show more

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Cited by 144 publications
(54 citation statements)
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“…3.2 for production of positive kaons in the pBe interactions. These were obtained through fits to data from [77,78,79,80,81,82,83,84]. Further details, including the full covariance matrices, can be found in [66].…”
Section: Neutrino Flux Predictionmentioning
confidence: 99%
See 1 more Smart Citation
“…3.2 for production of positive kaons in the pBe interactions. These were obtained through fits to data from [77,78,79,80,81,82,83,84]. Further details, including the full covariance matrices, can be found in [66].…”
Section: Neutrino Flux Predictionmentioning
confidence: 99%
“…The K + production model is based on a variety of experiments [77,78,79,80,81,82,83,84] using proton beams with momenta between 9.5 and 24 GeV/c. Feynman scaling is used to extrapolate these data to the 8.89 GeV/c Booster beam.…”
Section: Neutrino Flux Predictionmentioning
confidence: 99%
“…Existing production data from the HARP [129], E910 [130], and eight other kaon production experiments [131,132,133,134,135,136,137,138], as well as data from Abe et al [139] on neutral kaon production, available in slightly different (p Z ,p T ) parameter space than that relevant to MiniBooNE, are used in several parametrization fits in order to extrapolate the double-differential cross-sections in the (p Z ,p T ) parameter space relevant to MiniBooNE.…”
Section: Neutrino Flux Predictionmentioning
confidence: 99%
“…The custom physics model is described in detail in Refs. [125,50], and summarized as follows.Primary p − Be interactions at 8.9 GeV/c proton kinetic energy are parametrized in terms of double-differential inelastic cross-sections, [131,132,133,134,135,136,137,138] The multiplicity of each secondary species is obtained with respect to the total inelastic production cross-section by integrating the corresponding parametrized double-differential cross-sections over the MiniBooNE proton kinematic phase-space, accounting for other proton elastic and inelastic processes as well.Each generated secondary in the simulation is tracked through the beamline geometry until it decays (producing the neutrino beam) or gets absorbed. The simulation accounts for the effect of the magnetic horn, particle decays, as well as electromagnetic processes and hadronic interactions (both for primary protons and secondary particles) in the beamline geometry/materials, also defined within the simulation.…”
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confidence: 99%
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