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Top Quark Production and Asymmetry at Tevatron

Top Quark Production and Asymmetry at Tevatron. Yen-Chu Chen Fermi National Accelerator Laboratory On behalf of the CDF/D0 collaborations June 11-21, 2012 @HQL2012. Outline. The Top quark Tevatron summary The CDF/D0 experiments Top quark production Production asymmetry Conclusion.

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Top Quark Production and Asymmetry at Tevatron

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  1. Top Quark Production and Asymmetry at Tevatron Yen-Chu Chen Fermi National Accelerator Laboratory On behalf of the CDF/D0 collaborations June 11-21, 2012 @HQL2012

  2. Outline • The Top quark • Tevatron summary • The CDF/D0 experiments • Top quark production • Production asymmetry • Conclusion @ HQL 2012

  3. The Top quark • Properties • Standard Model • Charge : + 2/3 • Spin : 1/2 • Mass : A free parameter • Life time: ~10-25 s • Top quark pairs are produced via proton antiproton collisions at Tevatron. @ HQL 2012

  4. @ HQL 2012

  5. Tevatron Integrated luminosity @ HQL 2012

  6. The detectors D0 CDF

  7. Top quark physics  q' l  q _ W  Production of top quark b t  P P   X b t W  _  q' l  q _ @ HQL 2012

  8. _ t t decay channels used Di-lepton, DIL Lepton + Jets, LJ b b l ± l + Looking for secondary vertex _ b _ q’ b q l - @ HQL 2012

  9. B tagging via Secondary vertex (SVX) Efficiency Mistagging Efficiency Mistagging @ HQL 2012

  10. B tagging at D0 @ HQL 2012

  11. Top di-lepton event candidate 69.7 @ HQL 2012

  12. Top quark production _ _ • p p→ t t • s ~ 7.22 pb at √S = 1.96 TeV: • (NNLL, C. Schwinn, arXiv:1205.0988) • 90% qq→ t t; 10% gg→ t t _ _ _ _  … @ HQL 2012

  13. DIL event selection • Two high pT leptons • > 20 GeV (CDF), > 15 GeV(D0) • || < 2 • High missing ET due to the two neutrinos being missing in detection • Suppressing of Z boson events • High total transverse energy • Two or more jets @ HQL 2012

  14. Cross section using dilepton events, 5.1 fb-1 Mtop= 172.5 GeV/c2 @ HQL 2012

  15. Production cross section • DIL alone: (mtop=172.5 GeV) • = 7.36 +0.90 -0.79 (stat + syst +lumi) pb • Combined with LJ: • =7.56 +0.63–0.56 (stat+syst + lumi) pb @ HQL 2012

  16. @ HQL 2012

  17. @ HQL 2012

  18. Top production asymmetry • Differential cross section • Dependent on q2 and * Mttandy • There is asymmetry with respect to beamline _ @ HQL 2012

  19. Theoretical interest • Exotic gluons • massive chiral color • RS gluon • color sextets, anti-triplets • Intermediate Vector B´ • Z´, W´,… • … • Model building must contend with • total s in good agreement with SM • ds/dMtt in good agreement with SM @ HQL 2012

  20. Using the lepton + jets events CDF, full RUN II data, with good silicon, 8.7 fb-1 • high pT lepton (e/m) • Et/pt > 20 GeV (/c) • || < 1.0 • missing ET • Four or more jets • || < 2.0 • at least one b-tagged jet • || < 1.0 • 2498 events • 505±123 non-tt background • mostly W+jets b l ± _ b q’ q @ HQL 2012

  21. Top reconstruction @ HQL 2012

  22. _ Asymmetry in the tt rest frame ytt _ @ HQL 2012

  23. Asymmetryfor reconstructed tt _ @ HQL 2012

  24. _ Dependence on yttbackground subtracted @ HQL 2012

  25. Dependence on Mtt _ @ HQL 2012

  26. Afb in parton level • Using Unfolding Matrix to correct for the bias caused by acceptance of the detector/trigger and the reconstruction. • CDF, 8.7 fb-1 Afb = 0.162  0.047 • D0, 5.4 fb-1 Afb = 0.196  0.065 PRD 84, 112005 @ HQL 2012

  27. Conclusion • Both CDF and D0 have measured the total tt production cross section. The results are consistent between the two experiments and with the Standard Model. • Both CDF and D0 observe a large production asymmetry. • CDF observe dependence on the yttand Mtt. But the dependence on Mtt is not very strong at D0. • More studies from both CDF and D0 will come in the near future. • Differential cross section in terms of cos, etc. • Result from DIL channel _ _ _ @ HQL 2012

  28. Thank you!!! @ HQL 2012

  29. @ HQL 2012

  30. @ HQL 2012

  31. Asymmetry from backgroundis small but not zero! tt rest frame lab frame @ HQL 2012

  32. Expecting Higgs at LHC/ATLAS @ HQL 2012

  33. @ HQL 2012

  34. Top reconstruction @ HQL 2012

  35. Inclusive asymmetry Dy yh @ HQL 2012

  36. Apply to not b tagged sampleS:B = 0.3 tt frame lab frame @ HQL 2012

  37. Afb from di-lepton channel • In progress of blessing • Shows also strong asymmetry • Combining with the result from the lepton + jets channel and using full dataset we could reach 5 sigma, if this asymmetry is true. • Also some puzzles similar to lepton + jets result! • Such as smaller asymmetry in the not b tagged sample • Is this just statistical or is it telling us something that we are not aware of? @ HQL 2012

  38. Asymmetry categorized @ HQL 2012

  39. Separated by number of jets • data: the high mass asymmetry is significantly reduced for 5 jet events • the NLO QCD asymmetry has a strong Njet dependence @ HQL 2012

  40. In the lab frame • Cross check using ? @ HQL 2012

  41. Productionasymmetry • “Evidence for a Mass Dependent Forward-Backward Asymmetry in Top Quark Pair Production”, • “Wine & Cheese” at Fermilab, Jan. 7, 2011. • Paper submitted to PRD. • D0 also see similar effect. @ HQL 2012

  42. prior measurements • CDF, 1.9 fb-1 , inclusive, corrected to “parton-level” • tt rest frame • NLO QCD • lab (pp) frame • NLO QCD PRL 101, 202001 (2008) @ HQL 2012

  43. prior measurements • D0, inclusive, background subtracted “data-level” • tt rest frame 0.9 fb-1 4.3 fb-1 PRL 100, 142002 (2008) ICHEP 2010 @ HQL 2012

  44. Top charge asymmetry in QCD • Halzen, Hoyer, Kim; Brown, Sadhev, Mikaelian; Kuhn, Rodrigo; Ellis, Dawson, Nason; Almeida, Sterman, Vogelsang; Bowen, Ellis, Rainwater In t t rest frame: + AFB~ +10-12 % NLO C= - 1 C = +1 AFB~ -7 % NLO + C = + 1 C = -1 AFB~ 6 ± 1 % NLO @ HQL 2012

  45. Asymmetry in tt and pp frame _ _ • The asymmetry in the lab. Frame is reduced by the uncontrolled boost along the beamline: @ HQL 2012

  46. MC NLO study • MCFM NLO calculation at “parton level” • MC@NLO + CDFSIM • Pythia remains good approximation of SM truth sim + reco sim + reco +bkg @ HQL 2012

  47. Correction to parton level • Bin by bin in the histogram • Pj : parton level distribution • Aj: acceptance of the analysis • Sij: smearing of the reconstruction • Ti: top signal Ti = Sij x Aj x Pj • Bi: background • Di: data distribution Pj = Aj-1 x Sij-1 x (Di – Bi) @ HQL 2012

  48. Asymmetry is a function of ytt and Mtt @ HQL 2012

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