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Antos, J.; Aoki, M.; Azfar, F.; Azzi-Bacchetta, P.; Azzurri, P.; Barnett, B. A.; Bedeschi, F.; Bodek, A.; Bolshov, A.; Brubaker, E.; Busetto, G.; Castro, A.; Cerrito, L.; Ciocci, M. A.; Clark, A.; Cruz, A.; D’Auria, S.; D’Onofrio, M.; Ehlers, J.; Eusebi, R.; Giolo, K.; Glenzinski, D.; Goncharov, M.; González, O.; Gunay-Unalan, Z.; Haber, C.; Hahn, S. R.; Han, J. Y.; Hare, M.; Harris, R. M.; Hill, C. S.; Hirschbuehl, D.; Holloway, A.; Incandela, J.; Ivanov, A.; Jang, D.; Khotilovich, V.; Kim, S. B.; Kong, D. J.; Kraan, A.; Kreps, M.; Lannon, K.; Leonardo, N.; Lipeles, E.; Maki, T.; Malde, S.; Marino, C.; McFarland, K. S.; McIntyre, P.; Messina, A.; Miles, J.; Mitselmakher, G.; Miyamoto, A.; Mohr, B.; Fernandez, P. Movilla; Mülmenstädt, J.; Murat, P.; Nielsen, J.; Norniella, O.; Ogawa, T.; Oh, Y. D.; Okusawa, T.; Palencia, E.; Paoletti, R.; Papadimitriou, V.; Paramonov, A. A.; Pellett, D. E.; Piacentino, G.; Pinera, L.; Pitts, K.; Punzi, G.; Rahaman, A.; Reisert, B.; Rogers, E.; Rott, C.; Sabik, S.; Schlabach, P.; Shimojima, M.; Skiba, A.; Slaughter, A. J.; Soderberg, M.; Soha, A.; Spezziga, M.; Squillacioti, P.; Takeuchi, Y.; Thom, J.; Tipton, P.; Toback, D.; Torretta, D.; Tsuchiya, R.; Unverhau, T.; Uozumi, S.; Vataga, E.; Vine, T.; Vollrath, I.; Volobouev, I.; Wittich, P.; Yagil, A.; Yamaoka, J.; Yao, W. M.
Physical review. D, Particles, fields, gravitation, and cosmology, 08/2006, Letnik: 74, Številka: 3Journal Article
We describe a measurement of the top quark mass using events with two charged leptons collected by the CDF II detector from $p\bar{p}$ collisions with $\sqrt s = 1.96$ TeV at the Fermilab Tevatron. The likelihood in top mass is calculated for each event by convoluting the leading order matrix element describing $q\bar{q} \to t\bar{t} \to b\ell\nu_{\ell}\bar{b}\ell'\nu_{\ell'}$ with detector resolution functions. The presence of background events in the data sample is modeled using similar calculations involving the matrix elements for major background processes. In a data sample with integrated luminosity of 340 pb$^{-1}$, we observe 33 candidate events and measure $M_{top} = 165.2 \pm 6.1(\textrm{stat.}) \pm 3.4(\textrm{syst.}) \mathrm{~GeV}/c^2.$ This measurement represents the first application of this method to events with two charged leptons and is the most precise single measurement of the top quark mass in this channel.
