This experiment measured the neutron total and reaction cross sections at 5.0 Bev. Transmission measurements were made in good and poor geometry. The high-energy neutron beam was produced when the Bevatron circulating proton beam struck a copper target. Neutrons were identified by their production of pions in a beryllium block. The pions were then detected by a counter telescope including a gas {C} {C}{}erenkov counter. The threshold of this gas {C} {C}{}erenkov counter defined the mean effective neutron energy at 5.0±{}0.4 Bev, with the half-intensity points of the neutron energy distribution at 5.9 and 4.2 Bev. The cross sections measured for the various elements are (in millibarns): The 5-Bev total cross sections are 20% below the total cross-sections measured at 1.4 Bev by Coor et al., whereas the reaction cross sections remain essentially constant as a function of energy above 300 Mev. This behavior of the cross sections can be interpreted by a generalized diffraction theory developed by Glassgold and Grieder.
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Atkinson et al. (1961) studied this question.
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