4.7 Article

Measurement of the t(t)over-bar cross section in p(p)over-bar collisions at √s=1.96 TeV using dilepton events with a lepton plus track selection

Journal

PHYSICAL REVIEW D
Volume 79, Issue 11, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.79.112007

Keywords

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Funding

  1. U. S. Department of Energy and National Science Foundation
  2. Italian Istituto Nazionale di Fisica Nucleare
  3. Ministry of Education, Culture, Sports, Science and Technology of Japan
  4. Natural Sciences and Engineering Research Council of Canada
  5. National Science Council of the Republic of China
  6. Swiss National Science Foundation
  7. A. P. Sloan Foundation
  8. Bundesministerium fur Bildung und Forschung, Germany
  9. Korean Science and Engineering Foundation and the Korean Research Foundation
  10. Science and Technology Facilities Council and the Royal Society, United Kingdom
  11. Institut National de Physique Nucleaire et Physique des Particules/CNRS
  12. Russian Foundation for Basic Research
  13. Ministerio de Ciencia e Innovacion, and Programa Consolider-Ingenio 2010, Spain
  14. Slovak RD Agency
  15. Academy of Finland
  16. Science and Technology Facilities Council [PPA/A/S/2003/00461/2, PP/E000452/1, ST/H001069/1, PP/E000444/1, ST/H001077/1] Funding Source: researchfish
  17. STFC [PP/E000452/1, ST/H001069/1, ST/H001077/1] Funding Source: UKRI

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This paper reports a measurement of the cross section for the pair production of top quarks in p (p) over bar collisions at root s = 1.96 TeV at the Fermilab Tevatron. The data were collected from the CDF run II detector in a set of runs with a total integrated luminosity of 1.1 fb(-1). The cross section is measured in the dilepton channel, the subset of t (t) over bar events in which both top quarks decay through t -> Wb -> l nu b, where l = e, mu, or tau. The lepton pair is reconstructed as one identified electron or muon and one isolated track. The use of an isolated track to identify the second lepton increases the t (t) over bar acceptance, particularly for the case in which one W decays as W -> tau nu. The purity of the sample may be further improved at the cost of a reduction in the number of signal events, by requiring an identified b jet. We present the results of measurements performed with and without the request of an identified b jet. The former is the first published CDF result for which a b-jet requirement is added to the dilepton selection. In the CDF data there are 129 pretag lepton + track candidate events, of which 69 are tagged. With the tagging information, the sample is divided into tagged and untagged subsamples, and a combined cross section is calculated by maximizing a likelihood. The result is sigma(t (t) over bar) = 9.6 +/- 1.2(stat)(-0.5)(+0.6)(sys) +/- 0.6(lum) pb, assuming a branching ratio of BR(W -> l nu) = 10.8% and a top mass of m(t) = 175 GeV/c(2).

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