4.7 Article

Search for the Higgs boson in the H → WW → lvjj decay channel at √s=7 TeV with the ATLAS detector

Journal

PHYSICS LETTERS B
Volume 718, Issue 2, Pages 391-410

Publisher

ELSEVIER
DOI: 10.1016/j.physletb.2012.10.066

Keywords

ATLAS; LHC; Higgs; WW

Funding

  1. ANPCyT, Argentina
  2. YerPhI, Armenia
  3. ARC, Australia
  4. BMWF, 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, European Union
  25. ERC, European Union
  26. IN2P3-CNRS, France
  27. CEA-DSM/IRFU, France
  28. GNAS, Georgia
  29. BMBF, Germany
  30. DFG, Germany
  31. HGF, Germany
  32. MPG, Germany
  33. AvH Foundation, Germany
  34. GSRT, Greece
  35. ISF, Israel
  36. MINERVA, Israel
  37. GIF, Israel
  38. DIP, Israel
  39. Benoziyo Center, Israel
  40. INFN, Italy
  41. MEXT, Japan
  42. JSPS, Japan
  43. CNRST, Morocco
  44. FOM, Netherlands
  45. NWO, Netherlands
  46. RCN, Norway
  47. MNiSW, Poland
  48. GRICES, Portugal
  49. FCT, Portugal
  50. MERYS (MECTS), Romania
  51. MES of Russia, Russian Federation
  52. ROSATOM, Russian Federation
  53. JINR
  54. MSTD, Serbia
  55. MSSR, Slovakia
  56. ARRS, Slovenia
  57. MVZT, Slovenia
  58. DST/NRF, South Africa
  59. MICINN, 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. STFC [PP/E002757/1, ST/M000753/1, ST/I003142/1, ST/K000640/1, ST/H001026/1, ST/K501840/1, ST/H001093/1, ST/L001195/1, ST/I006080/1, ST/G502320/1, ST/J004928/1, PP/E000355/1, ST/H001042/1, ST/I005811/1, ST/L001144/1, ST/H00100X/1, ST/K000705/1, ST/K00140X/1, ST/F007337/1, ST/H001042/2, ST/J004944/1, PP/E003699/2, ST/M000761/1, ST/J005576/1, ST/H001069/2, ST/K001361/1, ST/I003525/1, ST/I005803/1, ST/J005460/1, PP/E003087/1, ST/I000186/1, ST/J002798/1, ST/K001329/1, ST/M001431/1, ST/H001093/2, ST/K001248/1, ST/K00073X/1, ST/M001512/1, PP/E003699/1, ST/H001026/2, ST/K001337/1, PP/E000347/1, ST/H00100X/2, ST/I003517/1] Funding Source: UKRI
  74. Science and Technology Facilities Council [ST/J005576/1, ST/K001310/1 LHCb Upgrades, ST/I000186/1, ST/K001337/1 ATLAS, ST/I006080/1, ST/J004928/1, PP/E003087/1, ST/I003517/1, ST/H00100X/2, ST/L001144/1, ST/K001310/1, PP/E003699/2, GRIDPP, ST/J005460/1, ST/K00073X/1, ST/K001361/1 LHCb, ST/J004928/1 ATLAS Upgrade, ST/K001310/1 LHCb, ST/K00140X/1, ST/H00100X/1, ST/J002798/1, ATLAS, ST/K001418/1, ST/J004944/1, ST/H001093/2, ST/K501840/1 GRIDPP, ST/G502320/1, PP/E003699/1, ST/M001431/1, ST/M001512/1, ST/K001248/1 ATLAS, PP/E000355/1, ST/K001361/1 ATLAS Upgrades, ST/K00140X/1 LHCb, ST/F007337/1, ST/K000705/1, ST/K001310/1 ATLAS Upgrades, ST/K001361/1 MINOS/MINOS+, ST/H001069/2, ST/H001026/1, ST/I005811/1, PP/E000347/1, ST/K001361/1 LHCb Upgrades, ST/H001042/1, ST/H001042/2, ST/H001093/1, ST/K001361/1, ST/K501840/1, ST/K001337/1, ST/K001264/1 ATLAS, ST/I005803/1 GRIDPP, ST/M000761/1, ST/K001248/1, ST/K001361/1 ATLAS, ST/K00140X/1 ATLAS, ST/L001195/1, ST/I003525/1, PP/E002757/1, ST/K001329/1 ATLAS, ST/I003142/1, ST/M001474/1, ST/I005803/1, ST/H001026/2, ST/K001310/1 ATLAS] Funding Source: researchfish
  75. Direct For Mathematical & Physical Scien
  76. Division Of Physics [1119200, 1056987] Funding Source: National Science Foundation
  77. ICREA Funding Source: Custom

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A search for the Standard Model Higgs boson has been performed in the H -> WW -> lvjj channel using 4.7 fb(-1) of pp collision data recorded at a centre-of-mass energy of root s = 7 TeV with the ATLAS detector at the Large Hadron Collider. Higgs boson candidates produced in association with zero, one or two jets are included in the analysis to maximize the acceptance for both gluon fusion and weak boson fusion Higgs boson production processes. No significant excess of events is observed over the expected background and limits on the Higgs boson production cross section are derived for a Higgs boson mass in the range 300 GeV < m(H) < 600 GeV. The best sensitivity is reached for m(H) = 400 GeV, where the observed (expected) 95% confidence level upper bound on the cross section for H -> WW produced in association with zero or one jet is 2.2 pb (1.9 pb), corresponding to 1.9 (1.6) times the Standard Model prediction. In the Higgs boson plus two jets channel, which is more sensitive to the weak boson fusion process, the observed (expected) 95% confidence level upper bound on the cross section for H -> WW production with m(H) = 400 GeV is 0.7 pb (0.6 pb), corresponding to 7.9 (6.5) times the Standard Model prediction. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved.

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