- Tytuł:
- Investigation of the $\Sigma ^{0}$ production mechanism in p(3.5 GeV)+p collisions
- Autorzy:
-
Krueger, W.
Zumbruch, P.
Zherebtsova, E.
Blanco, A.
Garzón, J. A.
Spies, S.
Galatyuk, T.
Kohls, M.
Przygoda, Witold
Korcyl, Grzegorz
Kunz, T.
Gumberidze, M.
Arnold, O.
Parpottas, Y.
Fröhlich, I.
Friese, J.
Kämpfer, B.
Pietraszko, J.
Dreyer, J.
Schild, N.
Svoboda, O.
Nowakowski, Krzysztof
Fabbietti, L.
Orliński, J.
Metag, V.
Hojeij, F.
Seck, F.
Idzik, M.
Michel, J.
Rathod, N.
Fonte, P.
Weber, A. A.
Chudoba, P.
Wendisch, C.
Markert, J.
Schwab, E.
Tlusty, P.
Molenda, A.
Koenig, I.
Höhne, C.
Kugler, A.
Pechenova, O.
Zieliński, Marcin
Kornakov, G.
Esmail, W.
Wagner, V.
Prozorov, A.
Koenig, W.
Lalik, Rafał
Kardan, B.
Nabroth, M.
Böhmer, M.
Stefaniak, M.
Huck, H.
Pechenov, V.
Kedych, V.
Malige, Akshay
Müntz, C.
Blume, C.
Carolino, N.
Salabura, Piotr
Grunwald, M.
Holzmann, R.
Bergmann, P.
Stroth, J.
Lopes, L.
Naumann, L.
Ritman, J.
Rustamov, A.
Sturm, C.
Tsertos, H.
Linz, F.
Piasecki, K.
Singh, Udai
Otto, J. -H.
Traxler, M.
Zbroszczyk, H. P.
Kotte, R.
Becker, M.
Ciepał, Izabela
Szala, M.
Chlad, L.
Ströbele, H.
Kolas, J.
Sumara, Konrad
Ramstein, B.
Lorenz, M.
Harabasz, S.
Yassine, R. Abou
Parschau, M.
Rost, A. - Opis:
- The production of $\Sigma^{0}$ hyperons in proton proton collisions at a beam kinetic energy of 3.5 GeV impinging on a liquid hydrogen target was investigated using data collected with the HADES setup. The total production cross section is found to be $\sigma(pK^{+} \Sigma^{0})$ = 17.7 $\pm$ 1.7(stat) $\pm$ 1.6(syst) μb. Differential cross section distributions of the exclusive channel $pp \to pK^{+} \Sigma^{0}$ were analyzed in the center-of-mass, Gottfried–Jackson and helicity reference frames for the first time at the excess energy of 556 MeV. The data support the interplay between pion and kaon exchange mechanisms and clearly demonstrate the contribution of interfering nucleon resonances decaying to $K^{+} \Sigma^{0}$. The Bonn–Gatchina partial wave analysis was employed to analyse the data. Due to the limited statistics, it was not possible to obtain an unambiguous determination of the relative contribution of intermediate nucleon resonances to the final state. However nucleon resonances with masses around 1.710 GeV/c$^{2}$ (N* (1710)) and 1.900 GeV/c$^{2}$ N* (1900) or $\Delta$* (1900)) are preferred by the fit.
- Dostawca treści:
- Repozytorium Uniwersytetu Jagiellońskiego
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