학술논문

Inclusive e$^+$e$^-$ production in collisions of pions with protons and nuclei in the second resonance region of baryons
Document Type
Working Paper
Author
Yassine, R. AbouAdamczewski-Musch, J.Arnold, O.Atomssa, E. T.Becker, M.Behnke, C.Berger-Chen, J. C.Blanco, A.Blume, C.Böhmer, M.Chlad, L.Chudoba, P.Ciepał, I.Deb, S.Deveaux, C.Dittert, D.Dreyer, J.Epple, E.Fabbietti, L.Fonte, P.Franco, C.Friese, J.Fröhlich, I.Förtsch, J.Galatyuk, T.Garzón, J. A.Gernhäuser, R.Greifenhagen, R.Grunwald, M.Gumberidze, M.Harabasz, S.Heinz, T.Hennino, T.Höhne, C.Hojeij, F.Holzmann, R.Idzik, M.Kämpfer, B.Kampert, K-H.Kardan, B.Kedych, V.Koenig, I.Koenig, W.Kohls, M.Kolas, J.Kolb, B. W.Korcyl, G.Kornakov, G.Kotte, R.Krueger, W.Kugler, A.Kunz, T.Lalik, R.Lapidus, K.Linev, S.Linz, F.Lopes, L.Lorenz, M.Mahmoud, T.Maier, L.Malige, A.Markert, J.Maurus, S.Metag, V.Michel, J.Mihaylov, D. M.Mikhaylov, V.Molenda, A.Müntz, C.Münzer, R.Nabroth, M.Naumann, L.Nowakowski, K.Orliński, J.Otto, J. -H.Parpottas, Y.Parschau, M.Pauly, C.Pechenov, V.Pechenova, O.Piasecki, K.Pietraszko, J.Povar, T.Prościnki, P.Prozorov, A.Przygoda, W.Pysz, K.Ramstein, B.Rathod, N.Rodriguez-Ramos, P.Rost, A.Rustamov, A.Salabura, P.Scheib, T.Schild, N.Schmidt-Sommerfeld, K.Schuldes, H.Schwab, E.Scozzi, F.Seck, F.Sellheim, P.Siebenson, J.Silva, L.Singh, U.Smyrski, J.Spataro, S.Spies, S.Stefaniak, M.Ströbele, H.Stroth, J.Sturm, C.Sumara, K.Svoboda, O.Szala, M.Tlusty, P.Traxler, M.Tsertos, H.Vazquez-Doce, O.Wagner, V.Weber, A. A.Wendisch, C.Wiebusch, M. G.Wirth, J.Wladyszewska, AZbroszczyk, H. P.Zherebtsova, E.Zielinski, M.Zumbruch, P.
Source
Subject
Nuclear Experiment
Language
Abstract
Inclusive e$^+$e$^-$ production has been studied with HADES in $\pi^-$ + p, $\pi^-$ + C and $\pi^- + \mathrm{CH}_2$ reactions, using the GSI pion beam at $\sqrt{s_{\pi p}}$ = 1.49 GeV. Invariant mass and transverse momentum distributions have been measured and reveal contributions from Dalitz decays of $\pi^0$, $\eta$ mesons and baryon resonances. The transverse momentum distributions are very sensitive to the underlying kinematics of the various processes. The baryon contribution exhibits a deviation up to a factor seven from the QED reference expected for the dielectron decay of a hypothetical point-like baryon with the production cross section constrained from the inverse $\gamma$ n$\rightarrow \pi^-$ p reaction. The enhancement is attributed to a strong four-momentum squared dependence of the time-like electromagnetic transition form factors as suggested by Vector Meson Dominance (VMD). Two versions of the VMD, that differ in the photon-baryon coupling, have been applied in simulations and compared to data. VMD1 (or two-component VMD) assumes a coupling via the $\rho$ meson and a direct coupling of the photon, while in VMD2 (or strict VMD) the coupling is only mediated via the $\rho$ meson. The VMD2 model, frequently used in transport calculations for dilepton decays, is found to overestimate the measured dielectron yields, while a good description of the data can be obtained with the VMD1 model assuming no phase difference between the two amplitudes. Similar descriptions have also been obtained using a time-like baryon transition form factor model where the pion cloud plays the major role.
Comment: (HADES collaboration)