par Trippe, Thomas;Windmolders, Roland;Slater, William W.E.;Bingham, Harry H.H.;Dunwoodie, W.;Drijard, Daniel;Linglin, D.;Goldschmidt-Clermont, Yves 
;Muller, Francis;Grard, Fernand ;Herquet, P. ;Naisse, Jacqueline ;Colton, Eugene;Schlein, Peter P.E.
Référence Nuclear physics. B, 41, 1, page (1-34)
Publication Publié, 1972-05
;Muller, Francis;Grard, Fernand ;Herquet, P. ;Naisse, Jacqueline ;Colton, Eugene;Schlein, Peter P.E.Référence Nuclear physics. B, 41, 1, page (1-34)
Publication Publié, 1972-05
Article révisé par les pairs
| Résumé : | Kπ scattering is studied in 77 300 bubble chamber events of K+p→K+π-π+p and 18800 events of K+p→Koπoπ+pfor beam momenta between 2.5 and 12.7 GeV/c. The on-shell moments of the angular distribution and the cross sections for K+π-→K+π-, K+π- →K0π0 and K+πo→Koπ+ are obtained by extrapolation to the pion pole. The same procedure applied to the π+p system correctly reproduces the known π+p scattering. A Kπ phase shift analysis between threshold and 1.1 GeV yields two solutions for the S wave isospin 1 2 phase shift (δ01). One solution gives a slowly increasing δ01 which approaches about 70° at 1.1 GeV. The other solution superposes on this behaviour a relatively narrow ({less-than or approximate} 30 MeV) resonant δ01 state near 890 MeV. Either case is compatible with a resonance in δ11 near 895 MeV and with a small, negative δ03. © 1972. |
