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@ARTICLE{Aad:588802,
      author       = {Aad, Georges and others},
      collaboration = {{ATLAS Collaboration}},
      title        = {{M}easurement of the top-quark mass using a leptonic
                      invariant mass in pp collisions at $ \sqrt{s} $ = 13 {T}e{V}
                      with the {ATLAS} detector},
      journal      = {Journal of high energy physics},
      volume       = {06},
      number       = {6},
      issn         = {1126-6708},
      address      = {[Trieste]},
      publisher    = {SISSA},
      reportid     = {PUBDB-2023-04959, arXiv:2209.00583. CERN-EP-2020-018},
      pages        = {19},
      year         = {2023},
      note         = {54 pages in total, author list starting page 37, 9 figures,
                      6 tables, published in JHEP 06 (2023) 019. All figures
                      including auxiliary figures are available at:
                      https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2017-17/},
      abstract     = {A measurement of the top-quark mass (m$_{t}$) in the $
                      t\overline{t} $ → lepton + jets channel is presented, with
                      an experimental technique which exploits semileptonic decays
                      of b-hadrons produced in the top-quark decay chain. The
                      distribution of the invariant mass m$_{ℓμ}$ of the
                      lepton, ℓ (with ℓ = e, μ), from the W-boson decay and
                      the muon, μ, originating from the b-hadron decay is
                      reconstructed, and a binned-template profile likelihood fit
                      is performed to extract m$_{t}$. The measurement is based on
                      data corresponding to an integrated luminosity of 36.1
                      fb$^{−1}$ of $ \sqrt{s} $ = 13 TeV pp collisions provided
                      by the Large Hadron Collider and recorded by the ATLAS
                      detector. The measured value of the top-quark mass is
                      m$_{t}$ = 174.41 ± 0.39 (stat.) ± 0.66 (syst.) ± 0.25
                      (recoil) GeV, where the third uncertainty arises from
                      changing the Pythia8 parton shower gluon-recoil scheme, used
                      in top-quark decays, to a recently developed setup.},
      keywords     = {p p: colliding beams (INSPIRE) / top: mass: measured
                      (INSPIRE) / top: decay (INSPIRE) / p p: scattering (INSPIRE)
                      / top: pair production (INSPIRE) / parton: showers (INSPIRE)
                      / final state: ((n)jet lepton) (INSPIRE) / ATLAS (INSPIRE) /
                      mass spectrum: (lepton muon) (INSPIRE) / bottom:
                      semileptonic decay (INSPIRE) / bottom: particle
                      identification (INSPIRE) / CERN LHC Coll (INSPIRE) / recoil
                      (INSPIRE) / data analysis method (INSPIRE) / numerical
                      calculations: Monte Carlo (INSPIRE) / experimental results
                      (INSPIRE) / 13000 GeV-cms (INSPIRE) / Hadron-Hadron
                      Scattering (autogen) / Top Physics (autogen)},
      cin          = {ATLAS},
      ddc          = {530},
      cid          = {I:(DE-H253)ATLAS-20120731},
      pnm          = {611 - Fundamental Particles and Forces (POF4-611)},
      pid          = {G:(DE-HGF)POF4-611},
      experiment   = {EXP:(DE-H253)LHC-Exp-ATLAS-20150101},
      typ          = {PUB:(DE-HGF)16},
      eprint       = {2209.00583},
      howpublished = {arXiv:2209.00583},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:2209.00583;\%\%$},
      UT           = {WOS:001035480600001},
      doi          = {10.1007/JHEP06(2023)019},
      url          = {https://bib-pubdb1.desy.de/record/588802},
}