The production of the J/ip meson by photons 1 was observed almost immediately after its discovery in hadronic 2 and electron-positron 3 collisions. The early measurements 1 " 4 focused on the extraction of the ^-nucleon total cross section with use of the vector dominance model. More recently, there have been several attempts to describe # photoproduction by means of constituent models such as photon-gluon fusion. 5 We have studied the production of ip mesons by photons up to the highest available energy, 300 GeV, incident on both liquid hydrogen and deuterium targets. In particular, we measure, in open geometry, the reactions y+(p or d) -ip (JU + M* °r e+e~) + X.(1)The Fermilab broad-band photon beam struck a 41-cm liquid target. Noninteracting photons traversed the detector, and deposited their energy in an integrating quantameter. Forward-going dilepton final states were detected in a multiparticle spectrometer, consisting of two analyzing mag-edited by T. Kirk and H.
Elastic scattering of hadrons on protons has been measured at momenta of 50, 100, and 200 GeV/c. The meson-proton scattering is found to be independent of momentum and meson type fort > 0.8 (GeV/c)'.The momentum dependence of the pp dip att = 1.4 (GeV/c)' was investigated. Slope parameters are given.
A resonance is observed in the diffractively photoproduced two-pion final state with a mass of ~ 1600 MeV and a width of ~ 300 MeV. The four-pion distribution is characterized by a width of ~ 600 MeV and peaks around 1500 MeV.The p'(1600) meson has been observed as an enhancement in the four-pion final state both in e + e~ collisions 1 and in photoproduction experiments. 2 "" 5 Estimates of the mass vary from 1430 to 1620 MeV, while estimates of the width vary from 310 to 650 MeV. A nonresonance interpretation of the photoproduction data as a purely kinematic enhancement in the pmi production amplitude also appears to describe these data adequately. 6 Indications of the existence of the two-pion decay mode have come from two photoproduction experiments 5 ' 7 and from a phase-shift analysis of the reaction n~p -+ir + Ti~n. 8 It has been assumed that the branching ratio of p'(1600) into two pions is small, although no published measurement of this number exists.We report here on a study of high-mass twoand four-pion final states photoproduced in the wide-band neutral beam at Fermilab. 9 Our expo-sure consisted of approximately 6 xlO 11 photons with energies greater than 50 GeV incident on a 2-cm-long (5% of a radiation length) scintillator target. The products of the interactions in the target were detected in the multiparticle spectrometer system described in Ref. 9. Two Cherenkov counters with pion thresholds of 6 and 12 GeV were used for particle indentification. A large lead-glass array detected y rays accompanying the charged particles. Two-pion events were recorded under a trigger designed to accept e + e~ pairs. The trigger had a finite efficiency for 7r + 7r pairs; however, uncertainties in the calculation of this efficiency result in a relatively large uncertainty in the absolute normalization for 77 + 7T states. Four-pion events were recorded under a trigger requiring at least three tracks in the spectrometer and a minimum energy deposition of 40 GeV in the hadron calorics)
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.