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  • Friedrich, S; Makonyi, K; Metag, V; Bayadilov, D; Bantes, B; Beck, R; Beloglazov, Y A; Böse, S; K -T Brinkmann; Challand, Th; Crede, V; Dahlke, T; Dietz, F; Drexler, P; Eberhardt, H; Elsner, D; Ewald, R; net-Ponse, K; Frommberger, F; Funke, Ch; Gottschall, M; Gridnev, A; Grüner, M; Gutz, E; Hammann, Ch; Hammann, D; Hannappel, J; Hartmann, J; Hillert, W; Hirenzaki, S; Hoffmeister, P; Honisch, Ch; Jaegle, I; Kaiser, D; Kalinowsky, H; Kammer, S; Keshelashvili, I; Kleber, V; Klein, F; Krusche, B; Lang, M; Lopatin, I V; Maghrbi, Y; Nanova, M; Nagahiro, H; Müller, J; Odenthal, T; Piontek, D; Rostomyan, T; Schaepe, S; Schmidt, Ch; Schmieden, H; Schmitz, R; Seifen, T; Thiel, A; Thoma, U; H van Pee; Walther, D; Weil, J; Wendel, Ch; Wiedner, U; Wilson, A; Winnebeck, A; Zenke, F; The CBELSA/TAPS Collaboration

    arXiv.org, 07/2014
    Paper

    In a search for \(\omega\) mesic states, the production of \(\omega\)-mesons in coincidence with forward going protons has been studied in photon induced reactions on \(^{12}\)C for incident photon energies of 1250 - 3100 MeV. The \(\pi^0 \gamma\) pairs from decays of bound or quasi-free \(\omega\)-mesons have been measured with the CBELSA/TAPS detector system in coincidence with protons registered in the MiniTAPS forward array. Structures in the total energy distribution of the \(\pi^0 \gamma\) pairs, which would indicate the population and decay of bound \(\omega~^{11}\)B states, are not observed. The \(\pi^0 \gamma\) cross section of 0.3 nb/MeV/sr observed in the bound state energy regime between -100 and 0 MeV may be accounted for by yield leaking into the bound state regime because of the large in-medium width of the \(\omega\)-meson. A comparison of the measured total energy distribution with calculations suggests the real part \(V_0\) of the \(\omega~^{11}\)B potential to be small and only weakly attractive with \(V_0(\rho=\rho_0) = -15\pm\) 35(stat) \(\pm\)20(syst) MeV in contrast to some theoretical predictions of attractive potentials with a depth of 100 - 150 MeV.