Anomaly detection search for new resonances decaying into a Higgs boson and a generic new particle X in hadronic final states using s=13 TeV pp collisions with the ATLAS detector

Aad, G.; Abbott, B.; Abbott, D. C.; Abeling, K.; Abidi, S. H.; Aboulhorma, A.; Abramowicz, H.; Abreu, H.; Abulaiti, Y.; Abusleme Hoffman, A. C.; Acharya, B. S.; Achkar, B.; Adam Bourdarios, C.; Adamczyk, L.; Adamek, L.; Addepalli, S. V.; Adelman, J.; Adiguzel, A.; Adorni, S.; Adye, T.; Affolder, A. A.; Afik, Y.; Agaras, M. N.; Agarwala, J.; Aggarwal, A.; Agheorghiesei, C.; Aguilar-Saavedra, J. A.; Ahmad, A.; Ahmadov, F.; Ahmed, W. S.; Ahuja, S.; Ai, X.; Aielli, G.; Aizenberg, I.; Akbiyik, M.; Åkesson, T. P. A.; Akimov, A. V.; Al Khoury, K.; Alberghi, G. L.; Albert, J.; Albicocco, P.; Alderweireldt, S.; Aleksa, M.; Aleksandrov, I. N.; Alexa, C.; Alexopoulos, T.; Alfonsi, A.; Alfonsi, F.; Alhroob, M.; Ali, B.; Ali, S.; Aliev, M.; Alimonti, G.; Alkakhi, W.; Allaire, C.; Allbrooke, B. M. M.; Allport, P. P.; Aloisio, A.; Alonso, F.; Alpigiani, C.; Alunno Camelia, E.; Alvarez Estevez, M.; Alviggi, M. G.; Aly, M.; Amaral Coutinho, Y.; Ambler, A.; Amelung, C.; Amerl, M.; Ames, C. G.; Amidei, D.; Amor Dos Santos, S. P.; Amoroso, S.; Amos, K. R.; Ananiev, V.; Anastopoulos, C.; Andeen, T.; Anders, J. K.; Andrean, S. Y.; Andreazza, A.; Angelidakis, S.; Angerami, A.; Anisenkov, A. V.; Annovi, A.; Antel, C.; Anthony, M. T.; Antipov, E.; Antonelli, M.; Antrim, D. J. A.; Anulli, F.; Aoki, M.; Aoki, T.; Aparisi Pozo, J. A.; Aparo, M. A.; Aperio Bella, L.; Appelt, C.; Aranzabal, N.; Araujo Ferraz, V.; Arcangeletti, C.; Arce, A. T. H.; Arena, E.; Arguin, J-F.; Argyropoulos, S.; Arling, J.H.; Armbruster, A. J.; Arnaez, O.; Arnold, H.; Arrubarrena Tame, Z. P.; Artoni, G.; Asada, H.; Asai, K.; Asai, S.; Asbah, N. A.; Assahsah, J.; Assamagan, K.; Astalos, R.; Atkin, R. J.; Atkinson, M.; Atlay, N. B.; Atmani, H.; Atmasiddha, P. A.; Augsten, K.; Auricchio, S.; Auriol, A. D.; Austrup, V. A.; Avner, G.; Avolio, G.; Axiotis, K.; Ayoub, M. K.; Azuelos, G.; Babal, D.; Bachacou, H.; Bachas, K.; Bachiu, A.; Backman, F.; Badea, A.; Bagnaia, P.; Bahmani, M.; Bailey, A. J.; Bailey, V. R.; Baines, J. T.; 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doi:10.1103/PhysRevD.108.052009
Anomaly detection search for new resonances decaying into a Higgs boson and a generic new particle $X$ in hadronic final states using $\sqrt{s} = 13 TeV$ $p p$ collisions with the ATLAS detector

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) ; D. C. Abbott (Department of Physics, University of Massachusetts, Amherst Massachusetts, USA) ; K. Abeling (II. Physikalisches Institut, Georg-August-Universität Göttingen, Göttingen, Germany) ; S. H. Abidi (Physics Department, Brookhaven National Laboratory, Upton New York, USA) ; et al. - Show all 2937 authors
A search is presented for a heavy resonance $Y$ decaying into a Standard Model Higgs boson $H$ and a new particle $X$ in a fully hadronic final state. The full Large Hadron Collider run 2 dataset of proton-proton collisions at $\sqrt{s} = 13 TeV$ collected by the ATLAS detector from 2015 to 2018 is used and corresponds to an integrated luminosity of $139 {fb}^{- 1}$ . The search targets the high $Y$ -mass region, where the $H$ and $X$ have a significant Lorentz boost in the laboratory frame. A novel application of anomaly detection is used to define a general signal region, where events are selected solely because of their incompatibility with a learned background-only model. It is constructed using a jet-level tagger for signal-model-independent selection of the boosted $X$ particle, representing the first application of fully unsupervised machine learning to an ATLAS analysis. Two additional signal regions are implemented to target a benchmark $X$ decay into two quarks, covering topologies where the $X$ is reconstructed as either a single large-radius jet or two small-radius jets. The analysis selects Higgs boson decays into $b \bar{b}$ , and a dedicated neural-network-based tagger provides sensitivity to the boosted heavy-flavor topology. No significant excess of data over the expected background is observed, and the results are presented as upper limits on the production cross section $σ (p p \to Y \to X H \to q \bar{q} b \bar{b}$ ) for signals with $m_{Y}$ between 1.5 and 6 TeV and $m_{X}$ between 65 and 3000 GeV.
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      "version_id": "333755e0-b55f-4311-a4d7-2f71184bc8b7", 
      "key": "10.1103/PhysRevD.108.052009.xml", 
      "size": 1089215
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  ], 
  "record_creation_date": "2023-09-18T20:30:07.091636", 
  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ex"
      ], 
      "value": "2306.03637"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "A search is presented for a heavy resonance <math><mi>Y</mi></math> decaying into a Standard Model Higgs boson <math><mi>H</mi></math> and a new particle <math><mi>X</mi></math> in a fully hadronic final state. The full Large Hadron Collider run 2 dataset of proton-proton collisions at <math><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math> collected by the ATLAS detector from 2015 to 2018 is used and corresponds to an integrated luminosity of <math><mn>139</mn><mtext> </mtext><mtext> </mtext><msup><mi>fb</mi><mrow><mo>\u2212</mo><mn>1</mn></mrow></msup></math>. The search targets the high <math><mi>Y</mi></math>-mass region, where the <math><mi>H</mi></math> and <math><mi>X</mi></math> have a significant Lorentz boost in the laboratory frame. A novel application of anomaly detection is used to define a general signal region, where events are selected solely because of their incompatibility with a learned background-only model. It is constructed using a jet-level tagger for signal-model-independent selection of the boosted <math><mi>X</mi></math> particle, representing the first application of fully unsupervised machine learning to an ATLAS analysis. Two additional signal regions are implemented to target a benchmark <math><mi>X</mi></math> decay into two quarks, covering topologies where the <math><mi>X</mi></math> is reconstructed as either a single large-radius jet or two small-radius jets. The analysis selects Higgs boson decays into <math><mi>b</mi><mover><mi>b</mi><mo>\u00af</mo></mover></math>, and a dedicated neural-network-based tagger provides sensitivity to the boosted heavy-flavor topology. No significant excess of data over the expected background is observed, and the results are presented as upper limits on the production cross section <math><mi>\u03c3</mi><mo>(</mo><mi>p</mi><mi>p</mi><mo>\u2192</mo><mi>Y</mi><mo>\u2192</mo><mi>X</mi><mi>H</mi><mo>\u2192</mo><mi>q</mi><mover><mi>q</mi><mo>\u00af</mo></mover><mi>b</mi><mover><mi>b</mi><mo>\u00af</mo></mover></math>) for signals with <math><msub><mi>m</mi><mi>Y</mi></msub></math> between 1.5 and 6 TeV and <math><msub><mi>m</mi><mi>X</mi></msub></math> between 65 and 3000 GeV."
    }
  ], 
  "imprints": [
    {
      "date": "2023-09-18", 
      "publisher": "APS"
    }
  ]
}
Published on:: 18 September 2023
Publisher:: APS
Published in:: Physical Review D , Volume 108 (2023)
Issue 5
DOI:: https://doi.org/10.1103/PhysRevD.108.052009
arXiv:: 2306.03637
Licence:: CC-BY-4.0
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