par Bassompierre, Gabriel;Perreau, J.-M.;Saitov, I.;Sekulin, R.;Wolf, Günter;De Baere, W.;Debaisieux, J.;Dufour, Pierre;Grard, Fernand 
;Heughebaert, Jacques ;Pape, Luc;Goldschmidt-Clermont, Yves ;Peeters, Philippe ;Verbeure, F;Windmolders, Roland;Jobes, M.;Matt, W.;Grant, A.;Henri, Victor;Hughes, I.;Jongejans, B.;Lander, R.L.;Linglin, D.;Muller, Francis
Référence Physics letters. Section B, 26, 1, page (30-34)
Publication Publié, 1967-12
;Heughebaert, Jacques ;Pape, Luc;Goldschmidt-Clermont, Yves ;Peeters, Philippe ;Verbeure, F;Windmolders, Roland;Jobes, M.;Matt, W.;Grant, A.;Henri, Victor;Hughes, I.;Jongejans, B.;Lander, R.L.;Linglin, D.;Muller, FrancisRéférence Physics letters. Section B, 26, 1, page (30-34)
Publication Publié, 1967-12
Article révisé par les pairs
| Résumé : | The study of K+p reactions at an incident momentum of 4.97 GeV/c suggests that the wide enhancement in the (Kππ)+ mass spectrum may be split into several resonant states. In particular, examination of the K*(892)π decay mode indicates the existence of the states K*(1230), K*(1280) and K*(1320), in addition to the well known K*(1420). The K*(1230) and K*(1320) have the properties expected from 1+ states produced by 0+ exchange. © 1967. |
