par Wittek, Wolfgang;Aderholz, M;Hantke, Detlev;Hoffmann, Ethan;Katz, Uli U.F.;Kern, J.;Schmitz, Norbert;Allport, P.P.;Cooper-Sarkar, Amanda A.M.;Guy, J. G V;Middleton, Robin R.P.;Venus, W.;Baton, J.P.;Neveu, Magella;Berggren, Mikael;Calicchio, Marco;Erriquez, Onofrio;Clayton, E.F. E.F.;Mobayyen, M.M. M.M.;Coghen, T.;Jones, G.T.;O'Neale, S.;Varvell, Kevin K.E.;Marage, Pierre
;Willocq, Stéphane;Matsinos, Evangelos;Simopoulou, E.;Vayaki, A.;Morrison, Douglas R O;Parker, Monique
;Wachsmuth, H.;Sansum, R.A. R.A.;Wells, James
Référence Zeitschrift für Physik. C, Particles and fields, 44, 2, page (175-186)
Publication Publié, 1989-06


Référence Zeitschrift für Physik. C, Particles and fields, 44, 2, page (175-186)
Publication Publié, 1989-06
Article révisé par les pairs
Résumé : | The production of the meson resonances ρ{variant}(770) (all three charge states), η(550), ω(783) and f2(1270) in {Mathematical expression} Ne and ν Ne charged current interactions is investigated in a bubble chamber experiment with BEBC at CERN. Except for the f2, the main features of resonance production are reasonably well described by the Lund model, although the average resonance multiplicities are overestimated by the model by (67±30)%. The average multiplicities of all resonances, including the f2, are well reproduced by a semiempirical model, whose parameters were determined from hadron interaction data. © 1989 Springer-Verlag. |