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Measurement of the top-quark mass in the all-hadronic channel using the full CDF data set

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Author(s)
Aaltonen, T.
Amerio, S.
Amidei, D.
Anastassov, A.
Annovi, A.
Antos, J.
Apollinari, G.
Appel, J. A.
Arisawa, T.
Artikov, A.
Asaadi, J.
Ashmanskas, W.
Auerbach, B.
Aurisano, A.
Azfar, F.
Badgett, W.
Bae, T.
Barbaro-Galtieri, A.
Barnes, V. E.
Barnett, B. A.
Barria, P.
Bartos, P.
Bauce, M.
Bedeschi, F.
Behari, S.
Bellettini, G.
Bellinger, J.
Benjamin, D.
Beretvas, A.
Bhatti, A.
Bland, K. R.
Blumenfeld, B.
Bocci, A.
Bodek, A.
Bortoletto, D.
Boudreau, J.
Boveia, A.
Brigliadori, L.
Bromberg, C.
Brucken, E.
Budagov, J.
Budd, H. S.
Burkett, K.
Busetto, G.
Bussey, P.
Butti, P.
Buzatu, A.
Calamba, A.
Camarda, S.
Campanelli, M.
Canelli, F.
Carls, B.
Carlsmith, D.
Carosi, R.
Carrillo, S.
Casal, B.
Casarsa, M.
Castro, A.
Catastini, P.
Cauz, D.
Cavaliere, V.
Cerri, A.
Cerrito, L.
Chen, Y. C.
Chertok, M.
Chiarelli, G.
Chlachidze, G.
Cho, K.
Chokheli, D.
Clark, A.
Clarke, C.
Convery, M. E.
Conway, J.
Corbo, M.
Cordelli, M.
Cox, C. A.
Cox, D. J.
Cremonesi, M.
Cruz, D.
Cuevas, J.
Culbertson, R.
d’Ascenzo, N.
Datta, M.
de Barbaro, P.
Demortier, L.
Deninno, M.
D’Errico, M.
Devoto, F.
Di Canto, A.
Di Ruzza, B.
Dittmann, J. R.
Donati, S.
D’Onofrio, M.
Dorigo, M.
Driutti, A.
Ebina, K.
Edgar, R.
Elagin, A.
Erbacher, R.
Errede, S.
Esham, B.
Farrington, S.
Fernández Ramos, J. P.
Field, R.
Flanagan, G.
Forrest, R.
Franklin, M.
Freeman, J. C.
Frisch, H.
Funakoshi, Y.
Galloni, C.
Garfinkel, A. F.
Garosi, P.
Gerberich, H.
Gerchtein, E.
Giagu, S.
Giakoumopoulou, V.
Gibson, K.
Ginsburg, C. M.
Giokaris, N.
Giromini, P.
Glagolev, V.
Glenzinski, D.
Gold, M.
Goldin, D.
Golossanov, A.
Gomez, G.
González López, O.
Gorelov, I.
Goshaw, A. T.
Goulianos, K.
Gramellini, E.
Grosso-Pilcher, C.
Group, R. C.
Guimaraes da Costa, J.
Hahn, S. R.
Han, J. Y.
Happacher, F.
Hara, K.
Hare, M.
Harr, R. F.
Harrington-Taber, T.
Hatakeyama, K.
Hays, C.
Heinrich, J.
Herndon, M.
Hocker, A.
Hong, Z.
Hopkins, W.
Hou, S.
Hughes, R. E.
Husemann, U.
Hussein, M.
Huston, J.
Introzzi, G.
Iori, M.
Ivanov, A.
James, E.
Jang, D.
Jayatilaka, B.
Jeon, E. J.
Jindariani, S.
Jones, M.
Joo, K. K.
Jun, S. Y.
Junk, T. R.
Kambeitz, M.
Kamon, T.
Karchin, P. E.
Kasmi, A.
Kato, Y.
Ketchum, W.
Keung, J.
Kilminster, B.
Kim, D. H.
Kim, H. S.
Kim, J. E.
Kim, M. J.
Kim, S. H.
Kim, S. B.
Kim, Y. J.
Kim, Y. K.
Kimura, N.
Kirby, M.
Knoepfel, K.
Kondo, K.
Kong, D. J.
Konigsberg, J.
Kotwal, A. V.
Kreps, M.
Kroll, J.
Kruse, M.
Kuhr, T.
Kurata, M.
Laasanen, A. T.
Lammel, S.
Lancaster, M.
Lannon, K.
Latino, G.
Lee, H. S.
Lee, J. S.
Leo, S.
Leone, S.
Lewis, J. D.
Limosani, A.
Lipeles, E.
Lister, A.
Liu, H.
Liu, Q.
Liu, T.
Lockwitz, S.
Loginov, A.
Lucchesi, D.
Lucà, A.
Lueck, J.
Lujan, P.
Lukens, P.
Lungu, G.
Lys, J.
Lysak, R.
Madrak, R.
Maestro, P.
Malik, S.
Manca, G.
Manousakis-Katsikakis, A.
Marchese, L.
Margaroli, F.
Marino, P.
Matera, K.
Mattson, M. E.
Mazzacane, A.
Mazzanti, P.
McNulty, R.
Mehta, A.
Mehtala, P.
Mesropian, C.
Miao, T.
Mietlicki, D.
Mitra, A.
Miyake, H.
Moed, S.
Moggi, N.
Moon, C. S.
Moore, R.
Morello, M. J.
Mukherjee, A.
Muller, Th.
Murat, P.
Mussini, M.
Nachtman, J.
Nagai, Y.
Naganoma, J.
Nakano, I.
Napier, A.
Nett, J.
Neu, C.
Nigmanov, T.
Nodulman, L.
Noh, S. Y.
Norniella, O.
Oakes, L.
Oh, S. H.
Oh, Y. D.
Oksuzian, I.
Okusawa, T.
Orava, R.
Ortolan, L.
Pagliarone, C.
Palencia, E.
Palni, P.
Papadimitriou, V.
Parker, W.
Pauletta, G.
Paulini, M.
Phillips, T. J.
Pianori, E.
Pilot, J.
Pitts, K.
Plager, C.
Pondrom, L.
Poprocki, S.
Potamianos, K.
Pranko, A.
Prokoshin, F.
Ptohos, F.
Punzi, G.
Redondo Fernández, I.
Renton, P.
Rescigno, M.
Rimondi, F.
Ristori, L.
Robson, A.
Rodriguez, T.
Rolli, S.
Ronzani, M.
Roser, R.
Rosner, J. L.
Ruffini, F.
Ruiz, A.
Russ, J.
Rusu, V.
Sakumoto, W. K.
Sakurai, Y.
Santi, L.
Sato, K.
Saveliev, V.
Savoy-Navarro, A.
Schlabach, P.
Schmidt, E. E.
Schwarz, T.
Scodellaro, L.
Scuri, F.
Seidel, S.
Seiya, Y.
Semenov, A.
Sforza, F.
Shalhout, S. Z.
Shears, T.
Shepard, P. F.
Shimojima, M.
Shochet, M.
Shreyber-Tecker, I.
Simonenko, A.
Sliwa, K.
Smith, J. R.
Snider, F. D.
Song, H.
Sorin, V.
St. Denis, R.
Stancari, M.
Stentz, D.
Strologas, J.
Sudo, Y.
Sukhanov, A.
Suslov, I.
Takemasa, K.
Takeuchi, Y.
Tang, J.
Tecchio, M.
Teng, P. K.
Thom, J.
Thomson, E.
Thukral, V.
Toback, D.
Tokar, S.
Tollefson, K.
Tomura, T.
Tonelli, D.
Torre, S.
Torretta, D.
Totaro, P.
Trovato, M.
Ukegawa, F.
Uozumi, S.
Vázquez, F.
Velev, G.
Vellidis, C.
Vernieri, C.
Vidal, M.
Vilar, R.
Vizán, J.
Vogel, M.
Volpi, G.
Wagner, P.
Wallny, R.
Wang, S. M.
Waters, D.
Wester, W. C.
Whiteson, D.
Wicklund, A. B.
Wilbur, S.
Williams, H. H.
Wilson, J. S.
Wilson, P.
Winer, B. L.
Wittich, P.
Wolbers, S.
Wolfe, H.
Wright, T.
Wu, X.
Wu, Z.
Yamamoto, K.
Yamato, D.
Yang, T.
Yang, U. K.
Yang, Y. C.
Yao, W.-M.
Yeh, G. P.
Yi, K.
Yoh, J.
Yorita, K.
Yoshida, T.
Yu, G. B.
Yu, I.
Zanetti, A. M.
Zeng, Y.
Zhou, C.
Zucchelli, S.
Gomez-Ceballos, Guillelmo
Goncharov, Maxim
Paus, Christoph M. E.
Date Issued
November 2014
Journal
Physical Review D
Publisher
American Physical Society
Citation
Aaltonen, T. et al. “Measurement of the Top-Quark Mass in the All-Hadronic Channel Using the Full CDF Data Set.” Physical Review D 90.9 (2014): n. pag. © 2014 American Physical Society
Version
Final published version
Abstract
The top-quark mass M[subscript top] is measured using top quark-antiquark pairs produced in proton-antiproton collisions at a center-of-mass energy of 1.96 TeV and that decay into a fully hadronic final state. The full data set collected with the CDF II detector at the Fermilab Tevatron Collider, corresponding to an integrated luminosity of 9.3  fb[superscript -1], is used. Events are selected that have six to eight jets, at least one of which is identified as having originated from a b quark. In addition, a multivariate algorithm, containing multiple kinematic variables as inputs, is used to discriminate signal events from background events due to QCD multijet production. Templates for the reconstructed top-quark mass are combined in a likelihood fit to measure M[subscript top] with a simultaneous calibration of the jet energy scale. A value of M[subscript top] = 175.07 ± 1.19(stat)  [+1.55 over -1.58](syst)  GeV/c[superscript 2] is obtained for the top-quark mass.
MIT Department
Massachusetts Institute of Technology. Laboratory for Nuclear Science
Terms of Use
Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.
Persistent DSpace Link
http://hdl.handle.net/1721.1/92278
DOI of Published Version
http://dx.doi.org/10.1103/PhysRevD.90.091101
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