4.4 Article

Search for charged Higgs bosons in the H± → tb decay channel in pp collisions at √s=8 TeV using the ATLAS detector

期刊

JOURNAL OF HIGH ENERGY PHYSICS
卷 -, 期 3, 页码 -

出版社

SPRINGER
DOI: 10.1007/JHEP03(2016)127

关键词

Hadron-Hadron scattering; Higgs physics

资金

  1. ANPCyT, Argentina
  2. YerPhI, Armenia
  3. ARC, Australia
  4. BMWFW, 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. IN2P3-CNRS, France
  26. CEA-DSM/IRFU, France
  27. GNSF, Georgia
  28. BMBF, Germany
  29. HGF, Germany
  30. MPG, Germany
  31. GSRT, Greece
  32. RGC, China
  33. Hong Kong SAR, China
  34. ISF, Israel
  35. I-CORE, Israel
  36. Benoziyo Center, Israel
  37. INFN, Italy
  38. MEXT, Japan
  39. JSPS, Japan
  40. CNRST, Morocco
  41. FOM, Netherlands
  42. NWO, Netherlands
  43. RCN, Norway
  44. MNiSW, Poland
  45. NCN, Poland
  46. FCT, Portugal
  47. MNE/IFA, Romania
  48. MES of Russia, Russian Federation
  49. NRC KI, Russian Federation
  50. JINR
  51. MESTD, Serbia
  52. MSSR, Slovakia
  53. ARRS, Slovenia
  54. MIZS, Slovenia
  55. DST/NRF, South Africa
  56. MINECO, Spain
  57. SRC, Sweden
  58. Wallenberg Foundation, Sweden
  59. SERI, Switzerland
  60. SNSF, Switzerland
  61. Cantons of Bern and Geneva, Switzerland
  62. MOST, Taiwan
  63. TAEK, Turkey
  64. STFC, United Kingdom
  65. DOE, United States of America
  66. NSF, United States of America
  67. BCKDF, Canada
  68. Canada Council, Canada
  69. CANARIE, Canada
  70. CRC, Canada
  71. Compute Canada, Canada
  72. FQRNT, Canada
  73. Ontario Innovation Trust, Canada
  74. EPLANET, European Union
  75. ERC, European Union
  76. FP7, European Union
  77. Horizon 2020, European Union
  78. Marie Sklodowska-Curie Actions, European Union
  79. Investissements d'Avenir Labex and Idex, France
  80. ANR, France
  81. Region Auvergne, France
  82. Fondation Partager le Savoir, France
  83. DFG, Germany
  84. AvH Foundation, Germany
  85. EU-ESF
  86. Greek NSRF
  87. BSF, Israel
  88. GIF, Israel
  89. Minerva, Israel
  90. BRF, Norway
  91. Royal Society, United Kingdom
  92. Leverhulme Trust, United Kingdom
  93. ICREA Funding Source: Custom
  94. Division Of Physics
  95. Direct For Mathematical & Physical Scien [1410972, 1506173, 1119200] Funding Source: National Science Foundation
  96. Science and Technology Facilities Council [ST/L001209/1 ATLAS Upgrades, ST/M007103/1 ATLAS Upgrades, PP/E000444/1, GRIDPP, ST/N000463/1, ST/M002071/1 ATLAS Upgrades, 1366825] Funding Source: researchfish
  97. STFC [ST/N000463/1] Funding Source: UKRI

向作者/读者索取更多资源

Charged Higgs bosons heavier than the top quark and decaying via H-+/- -> tb are searched for in proton-proton collisions measured with the ATLAS experiment at root s = 8 TeV corresponding to an integrated luminosity of 20.3 fb(-1). The production of a charged Higgs boson in association with a top quark, gb -> tH(+/-), is explored in the mass range 200 to 600 GeV using multi-jet final states with one electron or muon. In order to separate the signal from the Standard Model background, analysis techniques combining several kinematic variables are employed. An excess of events above the background only hypothesis is observed across a wide mass range, amounting to up to 2.4 standard deviations. Upper limits are set on the gb -> tH(+/-) production cross section times the branching fraction BR(H-+/- -> tb). Additionally, the complementary s-channel production, qq' -> H-+/-, is investigated through a reinterpretation of W' -> tb searches in ATLAS. Final states with one electron or muon are relevant for H-+/- masses from 0.4 to 2.0 TeV, whereas the all-hadronic final state covers the range 1.5 to 3.0 TeV. In these search channels, no significant excesses from the predictions of the Standard Model are observed, and upper limits are placed on the qq' -> H-+/- production cross section times the branching fraction BR(H-+/- -> tb).

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