1973
DOI: 10.1007/bf01394540
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Photoproduction of high-energy neutrons in thick targets by electrons in the energy range 150 to 270 MeV

Abstract: Photoneutron spectra with energies greater than 12 MeV produced by electrons incident on a thick lead target have been measured for primary electron energies between 150 and 266 MeV and at a fixed angle of 90 ~ to the beam axis. Measurements of the neutron yield have furthermore been performed at a primary energy of 234 MeV as a function of target depth for the same lead target and as a function of the mass number for C, A1, Cu, Cd and Pb targets. The results were obtained with three independent neutron detect… Show more

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Cited by 16 publications
(2 citation statements)
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“…Still, there were rather few studies which highlighted the quasi-deuteron mechanism as an important reaction mechanism in this energy region for electron beams. One example of high energy neutron production at 90 • was investigated for electron beam energies between 150 and 260 MeV by Eyss and Lührs at Mainz in 1973 [49]. Neutron production for 150-200 MeV was nicely accounted for by the quasi-deuteron based model by Matthews et al [50] while an additional neutron-production bump was observed for higher energy electrons due to the onset of pion-production channels.…”
Section: Interaction Of Electrons and Protons With Nucleimentioning
confidence: 99%
“…Still, there were rather few studies which highlighted the quasi-deuteron mechanism as an important reaction mechanism in this energy region for electron beams. One example of high energy neutron production at 90 • was investigated for electron beam energies between 150 and 260 MeV by Eyss and Lührs at Mainz in 1973 [49]. Neutron production for 150-200 MeV was nicely accounted for by the quasi-deuteron based model by Matthews et al [50] while an additional neutron-production bump was observed for higher energy electrons due to the onset of pion-production channels.…”
Section: Interaction Of Electrons and Protons With Nucleimentioning
confidence: 99%
“…Correction for the yields from the secondary reactions was performed on the basis of the excitation functions for these secondary reactions calculated with the ALICE code [24,25], the reported photoproton [26][27][28], and photoneutron spectra [29,30]. The details of the method as well as the Parameter evaluation for the calculation were described in Refs.…”
Section: Photopion Yieldsmentioning
confidence: 99%