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Título: | Erratum: Search for anomalous tt¯ production in the highly-boosted all-hadronic final state |
Autor: | Chatrchyan, S.; Brochero Cifuentes, J. A. CSIC ORCID; Cabrillo, I. J. CSIC ORCID ; Calderon, Alicia ; Chuang, S. H. CSIC; Duarte Campderros, J. CSIC ORCID ; Felcini, Marta CSIC ORCID; Fernández-García, Marcos CSIC ORCID ; Gómez, Gervasio CSIC ORCID ; González Sánchez, J. CSIC ; Jorda, C. CSIC; Lobelle Pardo, P. CSIC; López Virto, A. CSIC ORCID ; Marco, Jesús CSIC ORCID ; Marco, Rafael CSIC; Martínez-Rivero, Celso CSIC ORCID ; Matorras, Francisco CSIC ORCID ; Muñoz Sánchez, F. J. CSIC ORCID; Rodrigo, Teresa CSIC ORCID ; Rodríguez Marrero, Ana Y. CSIC; Ruiz Jimeno, Alberto CSIC ORCID ; Scodellaro, Luca CSIC ORCID ; Sobron Sañudo, M. CSIC; Vila, Iván CSIC ORCID; Vilar Cortabitarte, R. CSIC ORCID; Swanson, J. | Fecha de publicación: | 28-mar-2014 | Editor: | Springer Nature | Citación: | Journal of High Energy Physics 2014: 132 (2014) | Resumen: | The uncertainties on the mistagged NTMJ background include the statis- tical uncertainty on the sample after loose selection, to which the mistag probability is applied; the statistical uncertainty on the mistag proba- bility itself, ranging from < 1% at 1 TeV /c 2 to ≈ 10% at 3 TeV /c 2 ; and the systematic uncertainty on the mistag probability application, as de- scribed in section 3.3, which is in the range of 1 to 5% depending on the t ̄ t mass. The total background uncertainty is ≈ 5% for the low-mass region, dominated by the systematic uncertainty, and ≈ 100% for the high-mass region, dominated by statistical uncertainty associated with the sample after loose selection. | Descripción: | Chatrchyan, S. et al. | Versión del editor: | http://dx.doi.org/10.1007/JHEP03(2014)132 | URI: | http://hdl.handle.net/10261/96515 | DOI: | 10.1007/JHEP03(2014)132 | E-ISSN: | 1029-8479 |
Aparece en las colecciones: | (IFCA) Artículos |
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