4.7 Article

Search for bottom squark pair production in proton-proton collisions at √s=13 TeV with the ATLAS detector

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EUROPEAN PHYSICAL JOURNAL C
卷 76, 期 10, 页码 -

出版社

SPRINGER
DOI: 10.1140/epjc/s10052-016-4382-4

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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. IN2P3-CNRS, France
  25. CEA-DSM/IRFU, France
  26. GNSF, Georgia
  27. BMBF, Germany
  28. HGF, Germany
  29. MPG, Germany
  30. GSRT, Greece
  31. RGC, Hong Kong SAR, China
  32. ISF, Israel
  33. I-CORE, Israel
  34. Benoziyo Center, Israel
  35. INFN, Italy
  36. MEXT, Japan
  37. JSPS, Japan
  38. CNRST, Morocco
  39. FOM, Netherlands
  40. NWO, Netherlands
  41. RCN, Norway
  42. MNiSW, Poland
  43. NCN, Poland
  44. FCT, Portugal
  45. MNE/IFA, Romania
  46. MES of Russia
  47. NRC KI, Russian Federation
  48. JINR
  49. MESTD, Serbia
  50. MSSR, Slovakia
  51. ARRS, Slovenia
  52. MIZS, Slovenia
  53. DST/NRF, South Africa
  54. MINECO, Spain
  55. SRC, Sweden
  56. Wallenberg Foundation, Sweden
  57. SERI, Switzerland
  58. SNSF, Switzerland
  59. Cantons of Bern and 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
  66. Canada Council
  67. CANARIE
  68. CRC
  69. Compute Canada
  70. FQRNT
  71. Ontario InnovationTrust, Canada
  72. EPLANET
  73. ERC
  74. FP7
  75. Marie Sklodowska-Curie Actions, European Union
  76. Investissements d'Avenir Labex and Idex, France
  77. ANR, France
  78. Region Auvergne, France
  79. Fondation Partager le Savoir, France
  80. DFG, Germany
  81. AvH Foundation, Germany
  82. EU-ESF
  83. Greek NSRF
  84. BSF, Israel
  85. GIF, Israel
  86. Minerva, Israel
  87. BRF, Norway
  88. Generalitat de Catalunya, Spain
  89. Generalitat Valenciana, Spain
  90. Royal Society, United Kingdom
  91. Leverhulme Trust, United Kingdom
  92. ICREA Funding Source: Custom
  93. STFC [ST/N000277/1, ST/L003449/1, ST/K001329/1, ST/L006162/1, ST/J005533/1, ST/J004804/1, ST/N000420/1, ST/N000331/1, ST/N000463/1, ST/L000997/1, ST/M000753/1, ST/N000307/1] Funding Source: UKRI
  94. Science and Technology Facilities Council [ATLAS, ST/K001329/1, 1370879, ST/L003449/1, 1803433, GRIDPP, PP/E000444/1, ST/N000307/1, ST/N000331/1, ST/N000420/1, ST/N000277/1, ST/N000463/1, ST/M000753/1, ST/J005533/1, ST/L006162/1, ST/K001329/1 ATLAS, ST/L000997/1, 1366825, ST/J004804/1] Funding Source: researchfish
  95. Division Of Physics
  96. Direct For Mathematical & Physical Scien [1119200, 1410972] Funding Source: National Science Foundation
  97. Grants-in-Aid for Scientific Research [16H06489] Funding Source: KAKEN

向作者/读者索取更多资源

The result of a search for pair production of the supersymmetric partner of the Standard Model bottom quark ((b) over tilde (1)) is reported. The search uses 3.2 fb(-1) of pp collisions at root s = 13 TeV collected by the ATLAS experiment at the Large Hadron Collider in 2015. Bottom squarks are searched for in events containing large missing transverse momentum and exactly two jets identified as originating from b-quarks. No excess above the expected Standard Model background yield is observed. Exclusion limits at 95 % confidence level on the mass of the bottom squark are derived in phenomenological supersymmetric R-parity-conserving models in which the (b) over tilde (1) is the lightest squark and is assumed to decay exclusively via (b) over tilde (1) -> b (chi) over tilde (0)(1), where (chi) over tilde (0)(1) is the lightest neutralino. The limits significantly extend previous results; bottom squark masses up to 800 (840) GeV are excluded for the. (chi) over tilde (0)(1) mass below 360 (100) GeV whilst differences in mass above 100 GeV between the (b) over tilde (1) and the (chi) over tilde (0)(1) are excluded up to a (b) over tilde (1) mass of 500 GeV.

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