4.8 Article

Measurement of the Differential Cross Section dσ/d(cosθt) for Top-Quark Pair Production in p(p)over-bar Collisions at √s = 1.96 TeV

Journal

PHYSICAL REVIEW LETTERS
Volume 111, Issue 18, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.111.182002

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 World Class University Program
  10. National Research Foundation of Korea
  11. Science and Technology Facilities Council
  12. Royal Society, U. K.
  13. Russian Foundation for Basic Research
  14. Ministerio de Ciencia e Innovacion and Programa Consolider-Ingenio, Spain
  15. Slovak RD Agency
  16. Academy of Finland
  17. Australian Research Council (ARC)
  18. EU Community Marie Curie Fellowship [302103]
  19. Science and Technology Facilities Council [ST/K000195/1, ST/K000748/1, PP/E003699/2, ST/K00140X/1, ST/H001085/2, ST/K00137X/1, PP/E003699/1, ST/H001069/2, ST/H001085/1, ST/M001474/1, ST/L00335X/1, ST/J005568/1] Funding Source: researchfish
  20. STFC [ST/K000195/1, ST/K000748/1, ST/K00137X/1, PP/E003699/1, ST/L00335X/1, ST/H001085/1, ST/H001085/2, ST/H001069/2, ST/K00140X/1, PP/E003699/2, ST/J005568/1] Funding Source: UKRI
  21. ICREA Funding Source: Custom

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We report a measurement of the differential cross section d sigma = d(cos theta(t)) for top-quark pair production as a function of the top-quark production angle in proton-antiproton collisions at root s = 1.96 TeV. This measurement is performed using data collected with the CDF II detector at the Tevatron, corresponding to an integrated luminosity of 9.4 fb(-1). We employ the Legendre polynomials to characterize the shape of the differential cross section at the parton level. The observed Legendre coefficients are in good agreement with the prediction of the next-to-leading-order standard- model calculation, with the exception of an excess linear-term coefficient a(1) = 0.40 +/- 0.12, compared to the standard-model prediction of a(1) = 0.15(-0.03)(+0.07)

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