Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb1 of proton-proton collision data at s=13 TeV with the ATLAS detector

M. Aaboud (Faculté des Sciences, Université Mohamed Premier and LPTPM, Oujda, Morocco) ; G. Aad (CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France) ; B. Abbott (Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, Oklahoma, USA) ; O. Abdinov (Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan) ; B. Abeloos (LAL, Université Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay, France) ; et al. - Show all 2928 authors

Searches for new heavy resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons, are presented using a data sample corresponding to 36.1 fb1 of pp collisions at s=13 TeV collected during 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting bosonic decay modes in the qqqq, ννqq, νqq, qq, νν, νν, ν, , qqbb, ννbb, νbb, and bb final states are combined, searching for a narrow-width resonance. Likewise, analyses selecting the leptonic ν and final states are also combined. These two sets of analyses are then further combined. No significant deviation from the Standard Model predictions is observed. Three benchmark models are tested: a model predicting the existence of a new heavy scalar singlet, a simplified model predicting a heavy vector-boson triplet, and a bulk Randall-Sundrum model with a heavy spin-2 Kaluza-Klein excitation of the graviton. Cross section limits are set at the 95% confidence level using an asymptotic approximation and are compared with predictions for the benchmark models. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The data exclude a heavy vector-boson triplet with mass below 5.5 TeV in a weakly coupled scenario and 4.5 TeV in a strongly coupled scenario, as well as a Kaluza-Klein graviton with mass below 2.3 TeV.

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  "titles": [
    {
      "source": "APS", 
      "title": "Combination of searches for heavy resonances decaying into bosonic and leptonic final states using <math><mrow><mn>36</mn><mtext> </mtext><mtext> </mtext><msup><mrow><mi>fb</mi></mrow><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup></mrow></math> of proton-proton collision data at <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math> with the ATLAS detector"
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  "dois": [
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      "journal_issue": "5", 
      "year": 2018
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  "page_nr": [
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      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
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  "copyright": [
    {
      "holder": "CERN", 
      "statement": "\u00a9 2018 CERN, for the ATLAS Collaboration", 
      "year": "2018"
    }
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  "control_number": "42848", 
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      "value": "1808.02380"
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  "abstracts": [
    {
      "source": "APS", 
      "value": "Searches for new heavy resonances decaying into different pairings of <math><mi>W</mi></math>, <math><mi>Z</mi></math>, or Higgs bosons, as well as directly into leptons, are presented using a data sample corresponding to <math><mrow><mn>36.1</mn><mtext> </mtext><mtext> </mtext><msup><mrow><mi>fb</mi></mrow><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup></mrow></math> of <math><mi>p</mi><mi>p</mi></math> collisions at <math><mrow><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></mrow></math> collected during 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting bosonic decay modes in the <math><mi>q</mi><mi>q</mi><mi>q</mi><mi>q</mi></math>, <math><mi>\u03bd</mi><mi>\u03bd</mi><mi>q</mi><mi>q</mi></math>, <math><mo>\u2113</mo><mi>\u03bd</mi><mi>q</mi><mi>q</mi></math>, <math><mo>\u2113</mo><mo>\u2113</mo><mi>q</mi><mi>q</mi></math>, <math><mo>\u2113</mo><mi>\u03bd</mi><mo>\u2113</mo><mi>\u03bd</mi></math>, <math><mo>\u2113</mo><mo>\u2113</mo><mi>\u03bd</mi><mi>\u03bd</mi></math>, <math><mo>\u2113</mo><mi>\u03bd</mi><mo>\u2113</mo><mo>\u2113</mo></math>, <math><mo>\u2113</mo><mo>\u2113</mo><mo>\u2113</mo><mo>\u2113</mo></math>, <math><mi>q</mi><mi>q</mi><mi>b</mi><mi>b</mi></math>, <math><mi>\u03bd</mi><mi>\u03bd</mi><mi>b</mi><mi>b</mi></math>, <math><mo>\u2113</mo><mi>\u03bd</mi><mi>b</mi><mi>b</mi></math>, and <math><mo>\u2113</mo><mo>\u2113</mo><mi>b</mi><mi>b</mi></math> final states are combined, searching for a narrow-width resonance. Likewise, analyses selecting the leptonic <math><mo>\u2113</mo><mi>\u03bd</mi></math> and <math><mo>\u2113</mo><mo>\u2113</mo></math> final states are also combined. These two sets of analyses are then further combined. No significant deviation from the Standard Model predictions is observed. Three benchmark models are tested: a model predicting the existence of a new heavy scalar singlet, a simplified model predicting a heavy vector-boson triplet, and a bulk Randall-Sundrum model with a heavy spin-2 Kaluza-Klein excitation of the graviton. Cross section limits are set at the 95% confidence level using an asymptotic approximation and are compared with predictions for the benchmark models. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The data exclude a heavy vector-boson triplet with mass below 5.5 TeV in a weakly coupled scenario and 4.5 TeV in a strongly coupled scenario, as well as a Kaluza-Klein graviton with mass below 2.3 TeV."
    }
  ], 
  "imprints": [
    {
      "date": "2018-09-26", 
      "publisher": "APS"
    }
  ]
}
Published on:
26 September 2018
Publisher:
APS
Published in:
Physical Review D , Volume 98 (2018)
Issue 5
DOI:
https://doi.org/10.1103/PhysRevD.98.052008
arXiv:
1808.02380
Copyrights:
© 2018 CERN, for the ATLAS Collaboration
Licence:
CC-BY-4.0

Fulltext files: