Measurement of the top quark mass in the lepton + <?format ?> jets final state with the matrix element method
Measurement of the top quark mass in the lepton + jets final state with the matrix...
Abazov, V. M; Abbott, B. M; Abolins, M. M; Acharya, B. S; Adams, M. S; Adams, T. S; Agelou, M. S; Aguilo, E. S; Ahn, S. H; Ahsan, M. H; Alexeev, G. D; Alkhazov, G. D; Alton, A. D; Alverson, G. D; Alves, G. A; Anastasoaie, M. A; Andeen, T. A; Anderson, S. A; Andrieu, B. A; Anzelc, M. S; Arnoud, Y. S; Arov, M. S; Askew, A. S; Åsman, B. S; Assis Jesus, A. C; Atramentov, O. C; Autermann, C. C; Avila, C. C; Ay, C. C; Badaud, F. C; Baden, A. C; Bagby, L. C; Baldin, B. C; Bandurin, D. V; Banerjee, P. V; Banerjee, S. V; Barberis, E. V; Bargassa, P. V; Baringer, P. V; Barnes, C. V; Barreto, J. V; Bartlett, J. F; Bassler, U. F; Bauer, D. F; Beale, S. F; Bean, A. F; Begalli, M. F; Begel, M. F; Belanger-Champagne, C. F; Bellantoni, L. F; Bellavance, A. F; Benitez, J. A; Beri, S. B; Bernardi, G. B; Bernhard, R. B; Berntzon, L. B; Bertram, I. B; Besançon, M. B; Beuselinck, R. B; Bezzubov, V. A; Bhat, P. C; Bhatnagar, V. C; Binder, M. C; Biscarat, C. C; Black, K. M; Blackler, I. M; Blazey, G. M; Blekman, F. M; Blessing, S. M; Bloch, D. M; Bloom, K. M; Blumenschein, U. M; Boehnlein, A. M; Boeriu, O. M; Bolton, T. A; Borissov, G. A; Bos, K. A; Bose, T. A; Brandt, A. A; Brock, R. A; Brooijmans, G. A; Bross, A. A; Brown, D. A; Buchanan, N. J; Buchholz, D. J; Buehler, M. J; Buescher, V. J; Burdin, S. J; Burke, S. J; Burnett, T. H; Busato, E. H; Buszello, C. P; Butler, J. M; Calfayan, P. M; Calvet, S. M; Cammin, J. M; Caron, S. M; Carvalho, W. M; Casey, B. C; Cason, N. M; Castilla-Valdez, H. M; Chakrabarti, S. M; Chakraborty, D. M; Chan, K. M; Chandra, A. M; Charles, F. M; Cheu, E. M; Chevallier, F. M; Cho, D. K; Choi, S. K; Choudhary, B. K; Christofek, L. K; Claes, D. K; Clément, B. K; Clément, C. K; Coadou, Y. K; Cooke, M. K; Cooper, W. E; Coppage, D. E; Corcoran, M. E; Cousinou, M.-C. E; Cox, B. E; Crépé-Renaudin, S. E; Cutts, D. E; Ćwiok, M. E; da Motta, H. E; Das, A. E; Das, M. E; Davies, B. E; Davies, G. E; Davis, G. A; De, K. A; de Jong, P. A; de Jong, S. J; De La Cruz-Burelo, E. J; De Oliveira Martins, C. J; Degenhardt, J. D; Déliot, F. D; Demarteau, M. D; Demina, R. D; Demine, P. D; Denisov, D. D; Denisov, S. P; Desai, S. P; Diehl, H. T; Diesburg, M. T; Doidge, M. T; Dominguez, A. T; Dong, H. T; Dudko, L. V; Duflot, L. V; Dugad, S. R; Duggan, D. R; Duperrin, A. R; Dyer, J. R; Dyshkant, A. R; Eads, M. R; Edmunds, D. R; Edwards, T. R; Ellison, J. R; Elmsheuser, J. R; Elvira, V. D; Eno, S. D; Ermolov, P. D; Evans, H. D; Evdokimov, A. D; Evdokimov, V. N; Fatakia, S. N; Feligioni, L. N; Ferapontov, A. V; Ferbel, T. V; Fiedler, F. V; Filthaut, F. V; Fisher, W. V; Fisk, H. E; Fleck, I. E; Ford, M. E; Fortner, M. E; Fox, H. E; Fu, S. E; Fuess, S. E; Gadfort, T. E; Galea, C. F; Gallas, E. F; Galyaev, E. F; Garcia, C. F; Garcia-Bellido, A. F; Gardner, J. F; Gavrilov, V. F; Gay, A. F; Gay, P. F; Gelé, D. F; Gelhaus, R. F; Gerber, C. E; Gershtein, Y. E; Gillberg, D. E; Ginther, G. E; Gollub, N. E; Gómez, B. E; Goussiou, A. E; Grannis, P. D; Greenlee, H. D; Greenwood, Z. D; Gregores, E. M; Grenier, G. M; Gris, Ph. M; Grivaz, J.-F. M; Grünendahl, S. M; Grünewald, M. W; Guo, F. W; Guo, J. W; Gutierrez, G. W; Gutierrez, P. W; Haas, A. W; Hadley, N. J; Haefner, P. J; Hagopian, S. J; Haley, J. J; Hall, I. J; Hall, R. E; Han, L. E; Hanagaki, K. E; Hansson, P. E; Harder, K. E; Harel, A. E; Harrington, R. E; Hauptman, J. M; Hauser, R. M; Hays, J. M; Hebbeker, T. M; Hedin, D. M; Hegeman, J. G; Heinmiller, J. M; Heinson, A. P; Heintz, U. P; Hensel, C. P; Herner, K. P; Hesketh, G. P; Hildreth, M. D; Hirosky, R. D; Hobbs, J. D; Hoeneisen, B. D; Hoeth, H. D; Hohlfeld, M. D; Hong, S. J; Hooper, R. J; Houben, P. J; Hu, Y. J; Hubacek, Z. J; Hynek, V. J; Iashvili, I. J; Illingworth, R. J; Ito, A. S; Jabeen, S. S; Jaffré, M. S; Jain, S. S; Jakobs, K. S; Jarvis, C. S; Jenkins, A. S; Jesik, R. S; Johns, K. S; Johnson, C. S; Johnson, M. S; Jonckheere, A. S; Jonsson, P. S; Juste, A. S; Käfer, D. S; Kahn, S. S; Kajfasz, E. S; Kalinin, A. M; Kalk, J. M; Kalk, J. R; Kappler, S. R; Karmanov, D. R; Kasper, J. R; Kasper, P. R; Katsanos, I. R; Kau, D. R; Kaur, R. R; Kehoe, R. R; Kermiche, S. R; Khalatyan, N. R; Khanov, A. R; Kharchilava, A. R; Kharzheev, Y. M; Khatidze, D. M; Kim, H. M; Kim, T. J; Kirby, M. H; Klima, B. H; Kohli, J. M; Konrath, J.-P. M; Kopal, M. M; Korablev, V. M; Kotcher, J. M; Kothari, B. M; Koubarovsky, A. M; Kozelov, A. V; Kröninger, K. V; Krop, D. V; Kryemadhi, A. V; Kuhl, T. V; Kumar, A. V; Kunori, S. V; Kupco, A. V; Kurča, T. V; Kvita, J. V; Lammers, S. V; Landsberg, G. V; Lazoflores, J. V; Le Bihan, A.-C. V; Lebrun, P. V; Lee, W. M; Leflat, A. M; Lehner, F. M; Lesne, V. M; Leveque, J. M; Lewis, P. M; Li, J. M; Li, Q. Z; Lima, J. G; Lincoln, D. G; Linnemann, J. G; Lipaev, V. V; Lipton, R. V; Liu, Z. V; Lobo, L. V; Lobodenko, A. V; Lokajicek, M. V; Lounis, A. V; Love, P. V; Lubatti, H. J; Lynker, M. J; Lyon, A. L; Maciel, A. K; Madaras, R. J; Mättig, P. J; Magass, C. J; Magerkurth, A. J; Magnan, A.-M. J; Makovec, N. J; Mal, P. K; Malbouisson, H. B; Malik, S. B; Malyshev, V. L; Mao, H. S; Maravin, Y. S; Martens, M. S; McCarthy, R. S; Meder, D. S; Melnitchouk, A. S; Mendes, A. S; Mendoza, L. S; Merkin, M. S; Merritt, K. W; Meyer, A. W; Meyer, J. W; Michaut, M. W; Miettinen, H. W; Millet, T. W; Mitrevski, J. W; Molina, J. W; Mondal, N. K; Monk, J. K; Moore, R. W; Moulik, T. W; Muanza, G. S; Mulders, M. S; Mulhearn, M. S; Mundal, O. S; Mundim, L. S; Mutaf, Y. D; Nagy, E. D; Naimuddin, M. D; Narain, M. D; Naumann, N. A; Neal, H. A; Negret, J. P; Neustroev, P. P; Noeding, C. P; Nomerotski, A. P; Novaes, S. F; Nunnemann, T. F; O’Dell, V. F; O’Neil, D. C; Obrant, G. C; Oguri, V. C; Oliveira, N. C; Onoprienko, D. C; Oshima, N. C; Otec, R. C; Otero y Garzón, G. J; Owen, M. J; Padley, P. J; Parashar, N. J; Park, S.-J. J; Park, S. K; Parsons, J. K; Partridge, R. K; Parua, N. K; Patwa, A. K; Pawloski, G. K; Perea, P. M; Perez, E. M; Peters, K. M; Pétroff, P. M; Petteni, M. M; Piegaia, R. M; Piper, J. M; Pleier, M.-A. M; Podesta-Lerma, P. L; Podstavkov, V. M; Pogorelov, Y. M; Pol, M.-E. M; Pompoš, A. M; Pope, B. G; Popov, A. V; Potter, C. V; Prado da Silva, W. L; Prosper, H. B; Protopopescu, S. B; Qian, J. B; Quadt, A. B; Quinn, B. B; Rangel, M. S; Rani, K. J; Ranjan, K. J; Ratoff, P. N; Renkel, P. N; Reucroft, S. N; Rijssenbeek, M. N; Ripp-Baudot, I. N; Rizatdinova, F. N; Robinson, S. N; Rodrigues, R. F; Royon, C. F; Rubinov, P. F; Ruchti, R. F; Rud, V. I; Sajot, G. I; Sánchez-Hernández, A. I; Sanders, M. P; Santoro, A. P; Savage, G. P; Sawyer, L. P; Scanlon, T. P; Schaile, D. P; Schamberger, R. D; Scheglov, Y. D; Schellman, H. D; Schieferdecker, P. D; Schmitt, C. D; Schwanenberger, C. D; Schwartzman, A. D; Schwienhorst, R. D; Sekaric, J. D; Sengupta, S. D; Severini, H. D; Shabalina, E. D; Shamim, M. D; Shary, V. D; Shchukin, A. A; Shephard, W. D; Shivpuri, R. K; Shpakov, D. K; Siccardi, V. K; Sidwell, R. A; Simak, V. A; Sirotenko, V. A; Skubic, P. A; Slattery, P. A; Smith, R. P; Snow, G. R; Snow, J. R; Snyder, S. R; Söldner-Rembold, S. R; Song, X. R; Sonnenschein, L. R; Sopczak, A. R; Sosebee, M. R; Soustruznik, K. R; Souza, M. R; Spurlock, B. R; Stark, J. R; Steele, J. R; Stolin, V. R; Stone, A. R; Stoyanova, D. A; Strandberg, J. A; Strandberg, S. A; Strang, M. A; Strauss, M. A; Ströhmer, R. A; Strom, D. A; Strovink, M. A; Stutte, L. A; Sumowidagdo, S. A; Svoisky, P. A; Sznajder, A. A; Talby, M. A; Tamburello, P. A; Taylor, W. A; Telford, P. A; Temple, J. A; Tiller, B. A; Titov, M. A; Tokmenin, V. V; Tomoto, M. V; Toole, T. V; Torchiani, I. V; Towers, S. V; Trefzger, T. V; Trincaz-Duvoid, S. V; Tsybychev, D. V; Tuchming, B. V; Tully, C. V; Turcot, A. S; Tuts, P. M; Unalan, R. M; Uvarov, L. M; Uvarov, S. M; Uzunyan, S. M; Vachon, B. M; van den Berg, P. J; Van Kooten, R. J; van Leeuwen, W. M; Varelas, N. M; Varnes, E. W; Vartapetian, A. W; Vasilyev, I. A; Vaupel, M. A; Verdier, P. A; Vertogradov, L. S; Verzocchi, M. S; Villeneuve-Seguier, F. S; Vint, P. S; Vlimant, J.-R. S; Von Toerne, E. S; Voutilainen, M. S; Vreeswijk, M. S; Wahl, H. D; Wang, L. D; Wang, M. H; Warchol, J. H; Watts, G. H; Wayne, M. H; Weber, G. H; Weber, M. H; Weerts, H. H; Wermes, N. H; Wetstein, M. H; White, A. H; Wicke, D. H; Wilson, G. W; Wimpenny, S. J; Wobisch, M. J; Womersley, J. J; Wood, D. R; Wyatt, T. R; Xie, Y. R; Xuan, N. R; Yacoob, S. R; Yamada, R. R; Yan, M. R; Yasuda, T. R; Yatsunenko, Y. A; Yip, K. A; Yoo, H. D; Youn, S. W; Yu, C. W; Yu, J. W; Yurkewicz, A. W; Zatserklyaniy, A. W; Zeitnitz, C. W; Zhang, D. W; Zhao, T. W; Zhou, B. W; Zhu, J. W; Zielinski, M. W; Zieminska, D. W; Zieminski, A. W; Zutshi, V. W; Zverev, E. G
2006-11-01 00:00:00
We present a measurement of the top quark mass with the matrix element method in the lepton + <?format ?> jets final state. As the energy scale for calorimeter jets represents the dominant source of systematic uncertainty, the matrix element likelihood is extended by an additional parameter, which is defined as a global multiplicative factor applied to the standard energy scale. The top quark mass is obtained from a fit that yields the combined statistical and systematic jet energy scale uncertainty. Using a data set of <?format ?> 0.4 fb - 1 taken with the D0 experiment at Run II of the Fermilab Tevatron Collider, the mass of the top quark <?format ?>is measured using topological information to be: m top ℓ + jets ( topo ) = 169.2 - 7.4 + 5.0 ( stat + J E S ) - 1.4 + 1.5 ( syst ) GeV , and when information about identified b jets is included: m top ℓ + jets ( b -tag ) = 170.3 - 4.5 + 4.1 ( stat + J E S ) - 1.8 + 1.2 ( syst ) GeV . The measurements yield a jet energy scale consistent with the reference scale.
http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.pngPhysical Review DAmerican Physical Society (APS)http://www.deepdyve.com/lp/american-physical-society-aps/measurement-of-the-top-quark-mass-in-the-lepton-format-jets-final-gOfkUMQxUU
Measurement of the top quark mass in the lepton + <?format ?> jets final state with the matrix element method
We present a measurement of the top quark mass with the matrix element method in the lepton + <?format ?> jets final state. As the energy scale for calorimeter jets represents the dominant source of systematic uncertainty, the matrix element likelihood is extended by an additional parameter, which is defined as a global multiplicative factor applied to the standard energy scale. The top quark mass is obtained from a fit that yields the combined statistical and systematic jet energy scale uncertainty. Using a data set of <?format ?> 0.4 fb - 1 taken with the D0 experiment at Run II of the Fermilab Tevatron Collider, the mass of the top quark <?format ?>is measured using topological information to be: m top ℓ + jets ( topo ) = 169.2 - 7.4 + 5.0 ( stat + J E S ) - 1.4 + 1.5 ( syst ) GeV , and when information about identified b jets is included: m top ℓ + jets ( b -tag ) = 170.3 - 4.5 + 4.1 ( stat + J E S ) - 1.8 + 1.2 ( syst ) GeV . The measurements yield a jet energy scale consistent with the reference scale.
Journal
Physical Review D
– American Physical Society (APS)
To get new article updates from a journal on your personalized homepage, please log in first, or sign up for a DeepDyve account if you don’t already have one.
All DeepDyve websites use cookies to improve your online experience. They were placed on your computer when you launched this website. You can change your cookie settings through your browser.