4.4 Article

A search for t(t)over-bar resonances using lepton-plus-jets events in proton-proton collisions at √s=8 TeV with the ATLAS detector

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 8, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP08(2015)148

Keywords

Exotics; Hadron-Hadron Scattering; Top physics

Funding

  1. ANPCyT, Argentina
  2. YerPhI, Armenia
  3. ARC, Australia
  4. BMWFW, Austria
  5. ANAS, Azerbaijan
  6. SSTC, Belarus
  7. CNPq, Brazil
  8. FAPESP, Brazil
  9. NSERC, Canada
  10. NRC, Canada
  11. CFI, Canada
  12. CERN
  13. CONICYT, Chile
  14. CAS, China
  15. MOST, China
  16. NSFC, China
  17. COLCIENCIAS, Colombia
  18. MSMT CR, Czech Republic
  19. MPO CR, Czech Republic
  20. VSC CR, Czech Republic
  21. DNRF, Denmark
  22. DNSRC, Denmark
  23. Lundbeck Foundation, Denmark
  24. EPLANET
  25. ERC
  26. NSRF
  27. 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. RGC, China
  39. Hong Kong SAR, China
  40. ISF, Israel
  41. MINERVA, Israel
  42. GIF, Israel
  43. I-CORE, Israel
  44. Benoziyo Center, Israel
  45. INFN, Italy
  46. MEXT, Japan
  47. JSPS, Japan
  48. CNRST, Morocco
  49. FOM, Netherlands
  50. NWO, Netherlands
  51. BRF, Norway
  52. RCN, Norway
  53. MNiSW, Poland
  54. NCN, Poland
  55. GRICES, Portugal
  56. FCT, Portugal
  57. MNE/IFA, Romania
  58. MES of Russia, Russian Federation
  59. NRC KI, Russian Federation
  60. JINR
  61. MSTD, Serbia
  62. MSSR, Slovakia
  63. ARRS, Slovenia
  64. MIZ. S, Slovenia
  65. DST/NRF, South Africa
  66. MINECO, Spain
  67. SRC, Sweden
  68. Wallenberg Foundation, Sweden
  69. SER, Switzerland
  70. SNSF, Switzerland
  71. Cantons of Bern and Geneva, Switzerland
  72. NSC, Taiwan
  73. TAEK, Turkey
  74. STFC, United Kingdom
  75. Royal Society and Leverhulme Trust, United Kingdom
  76. DOE, United States of America
  77. NSF, United States of America
  78. ICREA Funding Source: Custom
  79. STFC [PP/E000355/1, ST/L003112/1, ST/I000178/1, PP/E003087/1, ST/I000186/1, ST/M004821/1, PP/D002915/1, ST/K50208X/1, ST/H00100X/1, ST/L001144/1, ST/H00100X/2, PP/E000347/1, ST/L006480/1, ST/I006056/1, ST/K00137X/1, ST/K00073X/1, ST/K001248/1, ST/G50228X/1, ST/H001093/2, ST/M001431/1, ST/K001329/1, ST/M001733/1, ST/K001388/1, ST/N000277/1, ST/K001361/1, ST/L000970/1, ST/M000664/1, ST/J005576/1, ST/M000761/1, ST/L00352X/1, ST/M503575/1, ST/M002306/1, ST/L003511/1, ST/K001302/1, ST/L003325/1, ST/J004944/1, ST/K00140X/1, ST/I005803/1, ST/M003213/1, ST/N000420/1, ST/M001504/1, ST/J00474X/1, ST/N000463/1, ST/J501074/1, ST/M006980/1, ST/M001407/1, ST/K000705/1, ST/J005525/1, ST/J005487/1, ST/N000307/1, ST/H001093/1, ST/L001195/1, ST/I006080/1, ST/G502320/1, ST/L003414/1, ST/L001179/1, ST/K003658/1, ST/I00372X/1, ST/J004928/1, PP/E002846/1] Funding Source: UKRI
  80. Science and Technology Facilities Council [ST/L000970/1 ATLAS Upgrades, ST/M004821/1 GRIDPP, ST/L003325/1, ST/I00372X/1, ST/J00474X/1, PP/E000347/1, ST/K001361/1 LHCb Upgrades, ST/L003112/1, ST/L00352X/1, ST/H001093/1, 1366825, ST/K001361/1, ST/K001302/1, ST/K001264/1 ATLAS, ST/I005803/1 GRIDPP, ST/M000761/1, ST/K001248/1, ST/K001361/1 ATLAS, ST/M003213/1, ST/G50228X/1, ST/L001195/1, ST/M001407/1, ST/M002306/1 ATLAS Upgrades, ST/L000970/1 ATLAS Upgrade, ST/K001396/1 ATLAS, ST/I000178/1, ST/K003658/1 GRIDPP, ST/M006980/1, ST/M002071/1 ATLAS Upgrades, 1521422, PP/D002915/1, ST/J005525/1, ST/M001474/1, ST/M000664/1, ST/J501074/1, ST/K003658/1, ST/L001179/1 ATLAS Upgrades, ST/M503575/1, ST/I005803/1, ST/L006480/1, ST/M007103/1 ATLAS Upgrades, ST/K001310/1 ATLAS, ST/K001361/1 MINOS/MINOS+, ST/I00372X/1 GRIDPP, ST/M001431/1, ST/G502320/1, ST/L001209/1 ATLAS Upgrades, ST/K00137X/1, ST/L001179/1, ST/N000463/1, ST/H001093/2, ST/L003414/1, ST/N000277/1, 1366364, ST/J004944/1, ST/M001504/1, ST/I006056/1, ST/K001418/1, ATLAS, ST/K001329/1, 1575161, ST/K000705/1, ST/N000420/1, ST/J005576/1, ST/K001310/1 LHCb Upgrades, ST/M006980/1 ATLAS Upgrades, ST/K001388/1, ST/I000186/1, ST/I006080/1, ST/N000307/1, ST/J004928/1, PP/E003087/1, ST/H00100X/2, ST/L001144/1, ST/M004821/1, PP/E002846/1, ST/M001733/1, ST/J00474X/1 ATLAS Upgrades, 1334588, ST/K001310/1, PP/E000444/1, 1201187, 1082012, GRIDPP, ST/K00073X/1, ST/M002306/1, ST/L001179/1 ATLAS Upgrade, ST/K001310/1 ATLAS Upgrades, ST/K001361/1 ATLAS Upgrades, ST/I006056/1 ATLAS Upgrade, ST/I006056/1 ATLAS Upgrades, PP/E000355/1, ST/K50208X/1, ST/J005487/1, ST/J004928/1 ATLAS Upgrades, ST/H00100X/1, ST/L000970/1, ST/K001361/1 LHCb, ST/J004928/1 ATLAS Upgrade, ST/L003511/1, ST/K001310/1 LHCb, ST/K001426/1 ATLAS, ST/K00140X/1] Funding Source: researchfish
  81. Direct For Mathematical & Physical Scien
  82. Division Of Physics [1506173, 1119200] Funding Source: National Science Foundation

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A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb(-1) of proton-proton collision data collected at a centre-of-mass energy of root s = 8TeV. The lepton-plus-jets final state is used, where the top pair decays to W (+) bW(-)(b) over bar, with one W boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow Z' boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour Z' boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with Gamma/m = 15% decaying to tt. These range from 4.8 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein excitation of the gluon in a Randall-Sundrum model is excluded for masses below 2.2 TeV.

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