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Babusci, D; Badoni, D; Balwierz-pytko, I; Bencivenni, G; Bini, C; Bloise, C; Bossi, F; Branchini, P; Budano, A; Caldeira Balkeståhl, L; Capon, G; Ceradini, F; Ciambrone, P; Czerwinski, E; Danè, E; De Lucia, E; De Robertis, G; De Santis, A; Di Domenico, A; Di Donato, C; Di Salvo, R; Domenici, D; Erriquez, O; Fanizzi, G; Fantini, A; Felici, G; Fiore, S; Franzini, P; Gauzzi, P; Giardina, G; Giovannella, S; Gonnella, F; Graziani, E; Happacher, F; Heijkenskjöld, L; Höistad, B; Iafolla, L; Jacewicz, M; Johansson, T; Kupsc, A; Lee-franzini, J; Leverington, B; Loddo, F; Loffredo, S; Mandaglio, G; Martemianov, M; Martini, M; Mascolo, M; Messi, R; Miscetti, S; Morello, G; Moricciani, D; Moskal, P; Nguyen, F; Passeri, A; Patera, V; Prado Longhi, I; Ranieri, A; Redmer, C F; Santangelo, P; Sarra, I; Schioppa, M; Sciascia, B; Silarski, M; Taccini, C; Tortora, L; Venanzoni, G; Wislicki, W; Wolke, M; Zdebik, J
The journal of high energy physics, 01/2013, Letnik: 2013, Številka: 1Journal Article
(ProQuest: ... denotes formulae and/or non-USASCII text omitted; see image) We present a measurement of eta meson production in photon-photon interactions produced by electron-positron beams colliding with ... GeV. The measurement is done with the KLOE detector at the -factory DAPhiNE with an integrated luminosity of 0.24 fb^sup -1^. The e ^sup +^ e ^sup -^ arrow right e ^sup +^ e ^sup -^ eta cross section is measured without detecting the out-going electron and positron, selecting the decays eta arrow right pi ^sup +^ pi ^sup -^ pi ^sup 0^ and eta arrow right pi ^sup 0^ pi ^sup 0^ pi ^sup 0^. The most relevant background is due to e ^sup +^ e ^sup -^ arrow right etaγ when the monochromatic photon escapes detection. The cross section for this process is measured as sigma(e ^sup +^ e ^sup -^ arrow right etaγ) = (856±8^sub stat^±16^sub syst^) pb. The combined result for the e ^sup +^ e ^sup -^ arrow right e ^sup +^ e ^sup -^ eta cross section is sigma(e ^sup +^ e ^sup -^ arrow right e ^sup +^ e ^sup -^ eta) = (32.72±1.27^sub stat^±0.70^sub syst^) pb. From this we derive the partial width Gamma(eta arrow right γγ) = (520±20^sub stat^±13^sub syst^) eV. This is in agreement with the world average and is the most precise measurement to date.
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