4.4 Article

Search for exotic decays of the Higgs boson into b(b)over-bar and missing transverse momentum in pp collisions at √s=13 TeV with the ATLAS detector

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 1, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP01(2022)063

Keywords

Hadron-Hadron scattering (experiments); Supersymmetry; Beyond Standard Model

Funding

  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. ANID, Chile
  15. CAS, China
  16. MOST, China
  17. NSFC, China
  18. Minciencias, Colombia
  19. MSMT CR, Czech Republic
  20. MPO CR, Czech Republic
  21. VSC CR, Czech Republic
  22. DNRF, Denmark
  23. DNSRC, Denmark
  24. IN2P3-CNRS, France
  25. CEA-DRF/IRFU, France
  26. SRNSFG, Germany
  27. Georgia, Germany
  28. BMBF, Germany
  29. HGF, Germany
  30. MPG, Germany
  31. GSRI, Greece
  32. RGC, China
  33. Hong Kong SAR, China
  34. ISF, Israel
  35. Benoziyo Center, Israel
  36. INFN, Italy
  37. MEXT, Japan
  38. JSPS, Japan
  39. CNRST, Morocco
  40. NWO, Netherlands
  41. RCN, Norway
  42. MEiN, Poland
  43. FCT, Portugal
  44. MNE/IFA, Romania
  45. JINR
  46. MES of Russia
  47. NRC KI, Russian Federation
  48. MESTD, Serbia
  49. MSSR, Slovakia
  50. ARRS, Slovenia
  51. MIZS, Slovenia
  52. DSI/NRF, South Africa
  53. MICINN, Spain
  54. SRC, Sweden
  55. Wallenberg Foundation, Sweden
  56. SERI, Switzerland
  57. SNSF, Switzerland
  58. Cantons of Bern, Switzerland
  59. Geneva, Switzerland
  60. MOST, Taiwan
  61. TAEK, Turkey
  62. STFC, United Kingdom
  63. DOE, United States of America
  64. NSF, United States of America
  65. BCKDF, Canada
  66. CANARIE, Canada
  67. Compute Canada, Canada
  68. CRC, Canada
  69. COST, European Union
  70. ERC, European Union
  71. ERDF, European Union
  72. Horizon 2020 and Marie Sklodowska-Curie Actions, European Union
  73. Investissements d'Avenir Labex, France
  74. Investissements d'Avenir Idex, France
  75. ANR, France
  76. DFG, Germany
  77. AvH Foundation, Germany
  78. Herakleitos, Thales
  79. EU-ESF, Greece
  80. Greek NSRF, Greece
  81. BSF-NSF, Israel
  82. GIF, Israel
  83. Norwegian Financial Mechanism 2014-2021, Norway
  84. NCN, Poland
  85. NAWA, Poland
  86. La Caixa Banking Foundation, Spain
  87. CERCA Programme Generalitat de Catalunya, Spain
  88. PROMETEO, Spain
  89. GenT Programmes Generalitat Valenciana, Spain
  90. Goran Gustafssons Stiftelse, Sweden
  91. Royal Society, United Kingdom
  92. Leverhulme Trust, United Kingdom
  93. Science and Technology Facilities Council [ST/S000879/1] Funding Source: researchfish

Ask authors/readers for more resources

This study describes the search for the exotic decay of the Higgs boson and sets upper limits on the product of cross section times branching ratio for a three-dimensional scan of the masses of the particles involved. The observations align with the predictions of the Standard Model, providing valuable insights for understanding particle physics and searching for new physics phenomena.
A search for the exotic decay of the Higgs boson (H) into a b (b) over bar resonance plus missing transverse momentum is described. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 fb(-1) of pp collisions at root s = 13 TeV. The search targets events from ZH production in an NMSSM scenario where H -> chi(similar to 0)(2)chi(similar to 0)(1), with chi(similar to 0)(2) -> a chi(similar to 0)(1), where a is a light pseudoscalar Higgs boson and chi(similar to 0)(1,)(2) are the two lightest neutralinos. The decay of the a boson into a pair of b-quarks results in a peak in the dijet invariant mass distribution. The final-state signature consists of two leptons, two or more jets, at least one of which is identified as originating from a b-quark, and missing transverse momentum. Observations are consistent with Standard Model expectations and upper limits are set on the product of cross section times branching ratio for a three-dimensional scan of the masses of the chi(similar to 0)(2), chi(similar to 0)(1) and a boson.

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