4.7 Article

Measurement of the t(t)over-bar production cross-section using eμ events with b-tagged jets in pp collisions at √s=7 and 8 TeV with the ATLAS detector

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EUROPEAN PHYSICAL JOURNAL C
卷 74, 期 10, 页码 -

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SPRINGER
DOI: 10.1140/epjc/s10052-014-3109-7

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资金

  1. ANPCyT, Argentina
  2. YerPhI, Armenia
  3. ARC, Australia
  4. BMWF, Austria
  5. FWF, Austria
  6. ANAS, Azerbaijan
  7. SSTC, Belarus
  8. CNPq, Brazil
  9. FAPESP, Brazil
  10. NSERC, Canada
  11. NRC, Canada
  12. CFI, Canada
  13. CERN
  14. CONICYT, Chile
  15. CAS, China
  16. MOST, China
  17. NSFC, China
  18. COLCIENCIAS, Colombia
  19. MSMT CR, Czech Republic
  20. MPO CR, Czech Republic
  21. VSC CR, Czech Republic
  22. DNRF, Denmark
  23. DNSRC, Denmark
  24. Lundbeck Foundation, Denmark
  25. EPLANET, European Union
  26. ERC, European Union
  27. NSRF, European Union
  28. IN2P3-CNRS, France
  29. CEA-DSM/IRFU, France
  30. GNSF, Georgia
  31. BMBF, Germany
  32. DFG, Germany
  33. HGF, Germany
  34. MPG, Germany
  35. AvH Foundation, Germany
  36. GSRT, Greece
  37. NSRF, Greece
  38. ISF, Israel
  39. MINERVA, Israel
  40. GIF, Israel
  41. I-CORE, Israel
  42. Benoziyo Center, Israel
  43. INFN, Italy
  44. MEXT, Japan
  45. JSPS, Japan
  46. CNRST, Morocco
  47. FOM, Netherlands
  48. NWO, Netherlands
  49. BRF, Norway
  50. RCN, Norway
  51. MNiSW, Poland
  52. NCN, Poland
  53. GRICES, Portugal
  54. FCT, Portugal
  55. MNE/IFA, Romania
  56. MES of Russia
  57. ROSATOM, Russian Federation
  58. JINR
  59. MINECO, Spain
  60. SRC, Sweden
  61. Wallenberg Foundation, Sweden
  62. SER, Switzerland
  63. SNSF, Switzerland
  64. Canton of Bern, Switzerland
  65. Canton of Geneva, Switzerland
  66. NSC, Taiwan
  67. TAEK, Turkey
  68. STFC, United Kingdom
  69. Royal Society, United Kingdom
  70. Leverhulme Trust, United Kingdom
  71. DOE, United States of America
  72. NSF, United States of America
  73. MSTD, Serbia
  74. MSSR, Slovakia
  75. ARRS, Slovenia
  76. MIZS, Slovenia
  77. DST/NRF, South Africa
  78. ICREA Funding Source: Custom
  79. STFC [PP/D002915/1, ST/H00100X/1, PP/E000355/1, ST/K50208X/1, PP/E002846/1, ST/J004928/1, ST/I00372X/1, ST/K003658/1, ST/L001179/1, ST/G502320/1, PP/E000487/1, ST/I006080/1, ST/L001195/1, ST/F00754X/1, ST/L006464/1, ST/H001026/1, ST/J005487/1, ST/J005525/1, ST/F007418/1, ST/H00095X/1, ST/K000705/1, ST/J501074/1, ST/J00474X/1, ST/M003213/1, ST/K00140X/1, ST/J004944/1, ST/L003325/1, ST/K001388/1, ST/K001302/1, ST/L003511/1, ST/M002306/1, ST/L00352X/1, ST/M000761/1, ST/J005576/1, ST/H001069/2, ST/K000713/1, ST/M000664/1, ST/L000970/1, ST/H00095X/2, ST/I005803/1, PP/E003087/1, ST/I000186/1, ST/L003112/1, ST/I000178/1, ST/M001733/1, ST/J002798/1, ST/K001329/1, ST/K502236/1, ST/I505756/1, ST/G50228X/1, ST/K001248/1, ST/K00137X/1, ST/I006056/1, ST/M001512/1, ST/H001026/2, ST/L006480/1, ST/H00100X/2] Funding Source: UKRI
  80. Division Of Physics
  81. Direct For Mathematical & Physical Scien [1119200] Funding Source: National Science Foundation
  82. Science and Technology Facilities Council [ST/J004944/1, ST/I006056/1, ST/K001418/1, ATLAS, ST/K001329/1, ST/K00140X/1, ST/K001426/1 ATLAS, ST/K001310/1 LHCb, ST/L003511/1, ST/J004928/1 ATLAS Upgrade, ST/L000970/1, ST/F007418/1, ST/H00100X/1, ST/J002798/1, ST/J005487/1, ST/K50208X/1, PP/E000355/1, ST/I006056/1 ATLAS Upgrades, ST/I006056/1 ATLAS Upgrade, ST/K001310/1 ATLAS Upgrades, ST/L001179/1 ATLAS Upgrade, ST/M002306/1, ST/I505756/1, GRIDPP, ST/L006464/1, ST/K001310/1, ST/F00754X/1, ST/J00474X/1 ATLAS Upgrades, ST/M001733/1, PP/E002846/1, ST/H00100X/2, PP/E003087/1, ST/J004928/1, ST/I006080/1, ST/K001337/1 ATLAS, ST/I000186/1, ST/K001388/1, ST/K001310/1 LHCb Upgrades, ST/J005576/1, ST/K000705/1, ST/K502236/1, ST/K000713/1, ST/L003325/1, ST/I00372X/1, ST/J00474X/1, ST/L003112/1, ST/L00352X/1, ST/K001302/1, ST/K001264/1 ATLAS, ST/H00095X/2, ST/I005803/1 GRIDPP, ST/M000761/1, ST/K001248/1, ST/K00140X/1 ATLAS, ST/M003213/1, ST/G50228X/1, ST/L001195/1, ST/H00095X/1, ST/L001179/1, ST/K00137X/1, ST/L001209/1 ATLAS Upgrades, ST/G502320/1, ST/M001512/1, ST/I00372X/1 GRIDPP, ST/H001026/1, ST/H001069/2, ST/K001310/1 ATLAS, ST/H001026/2, ST/M007103/1 ATLAS Upgrades, ST/L006480/1, ST/I005803/1, ST/L001179/1 ATLAS Upgrades, ST/K003658/1, ST/J501074/1, ST/M000664/1, ST/M001474/1, ST/J005525/1, PP/E000487/1, PP/D002915/1, ST/M002071/1 ATLAS Upgrades, ST/K003658/1 GRIDPP, ST/I000178/1, ST/L000970/1 ATLAS Upgrade, ST/M002306/1 ATLAS Upgrades] Funding Source: researchfish

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The inclusive top quark pair (t (t) over tilde) production cross-section sigma(t (t) over bar) has been measured in proton-proton collisions at root s = 7 TeV and root s = 8 TeV with the ATLAS experiment at the LHC, using t (t) over bar events with an opposite-charge e mu pair in the final state. The measurement was performed with the 2011 7 TeV dataset corresponding to an integrated luminosity of 4.6 fb(-1) and the 2012 8 TeV dataset of 20.3 fb(-1). The numbers of events with exactly one and exactly two b-tagged jets were counted and used to simultaneously determine sigma(t (t) over bar) and the efficiency to reconstruct and b-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section was measured to be: sigma(t (t) over bar) = 182.9 +/- 3.1 +/- 4.2 +/- 3.6 +/- 3.3 pb (root s = 7 TeV) and sigma(t (t) over bar) = 242.4 +/- 1.7 +/- 5.5 +/- 7.5 +/- 4.2 pb (root s = 8 TeV), where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, knowledge of the integrated luminosity and of the LHC beam energy. The results are consistent with recent theoretical QCD calculations at next-to-next-to-leading order. Fiducial measurements corresponding to the experimental acceptance of the leptons are also reported, together with the ratio of cross-sections measured at the two centre-of-mass energies. The inclusive cross-section results were used to determine the top quark pole mass via the dependence of the theoretically predicted cross-section on m(t)(pole) giving a result of m(t)(pole) = 172.9(-2.6)(+2.5) GeV. By looking for an excess of t (t) over bar production with respect to the QCD prediction, the results were also used to place limits on the pair-production of supersymmetric top squarks (t) over tilde (1) with masses close to the top quarkmass, decaying via (t) over tilde (1) -> t (chi) over tilde (0)(1) 1 to predominantly right-handed top quarks and a light neutralino (chi) over tilde (0)(1) 1, the lightest supersymmetric particle. Top squarks with masses between the top quark mass and 177 GeV are excluded at the 95% confidence level.

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