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Bassalleck, B; Berdoz, A; Bradtke, C; Bröders, R; Bunker, B; Dennert, H; Dutz, H; Eilerts, S; Eyrich, W; Fields, D; Fischer, H; Franklin, G; Franz, J; Gehring, R; Geyer, R; Goertz, S; Hamann, N; Harmsen, J; Hauffe, J; Heinsius, F; Hertzog, D; Johansson, T; Jones, T; Khaustov, P; Kilian, K; Kingsberry, P; Kriegler, E; Lowe, J; Meier, A; Metzger, A; Meyer, C; Meyer, W; Moosburger, M; Oelert, W; Paschke, K; Plückthun, M; Pomp, S; Quinn, B; Reicherz, G; Röhrich, K; Sachs, K; Schmitt, H; Schoch, B; Sefzick, T; Stinzing, F; Stotzer, R; Tayloe, R; Wirth, St
Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms, 2004, 2004-1-00, Letnik: 214Journal Article
The reaction p p→ Λ Λ was examined by LEAR experiment PS185/3 at 1.525 and 1.640 GeV/c. The proton target was transversely polarized in order to measure the depolarization and spin transfer. Theoretical calculations of D nn, the component of the depolarization normal to the production plane, differ greatly according to whether quark-gluon or meson-exchange models are employed. The measured D nn and spin transfer K nn appear to be inconsistent with the specific models cited.
