% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Aad:187268,
      author       = {Aad, Georges and others},
      collaboration = {{ATLAS Collaboration}},
      title        = {{M}easurement of the top-quark mass in the fully hadronic
                      decay channel from {ATLAS} data at $\sqrt{s}=7$ {T}e{V}},
      reportid     = {PUBDB-2014-03836, CERN-PH-EP-2014-208. arXiv:1409.0832},
      year         = {2014},
      note         = {14 pages plus author list + cover pages (28 pages total), 6
                      figures, 4 tables, submitted to Eur. Phys. J. C 02.09.2014.
                      All figures, including auxiliary figures, are available at
                      http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2013-03/},
      abstract     = {The mass of the top quark is measured in a data set
                      corresponding to 4.6 fb$^{-1}$ of proton-proton collisions
                      with centre-of-mass energy $\sqrt{s}=7$ TeV collected by the
                      ATLAS detector at the LHC. Events consistent with hadronic
                      decays of top-antitop quark pairs with at least six jets in
                      the final state are selected. The substantial background
                      from multijetproduction is modelled with data-driven methods
                      that utilise the number of identified $b$-quark jets and the
                      transverse momentum of the sixth leading jet,which have
                      minimal correlation. The top-quark mass is obtained from
                      template fits to the ratio of three-jet to dijet mass. The
                      three-jet mass is calculated from the three jets produced in
                      a top-quark decay. Using these three jets the dijet mass is
                      obtained from the two jets produced in the $W$ boson decay.
                      The top-quark mass obtained from this fit is thus less
                      sensitive to the uncertainty in the energy measurement of
                      the jets. A binned likelihood fit yields a top-quark mass of
                      $m_{t} = 175.1 \pm 1.4$ (stat) $\pm 1.2$ (syst) GeV.},
      keywords     = {p p: scattering (INSPIRE) / top: pair production (INSPIRE)
                      / top: mass: measured (INSPIRE) / bottom: particle
                      identification (INSPIRE) / jet: multiplicity (INSPIRE) /
                      mass: (3jet) (INSPIRE) / dijet: mass (INSPIRE) / mass ratio
                      (INSPIRE) / data analysis method (INSPIRE) / experimental
                      results (INSPIRE) / ATLAS (INSPIRE) / CERN LHC Coll
                      (INSPIRE) / 7000 GeV-cms (INSPIRE)},
      cin          = {ATLAS},
      cid          = {I:(DE-H253)ATLAS-20120731},
      pnm          = {Experiments at LHC (ATLAS) (POF2-512)},
      pid          = {G:(DE-H253)POF2-LHC-Exp.-(ATLAS)-20130405},
      experiment   = {EXP:(DE-H253)LHC-Exp-ATLAS-20150101},
      typ          = {PUB:(DE-HGF)25 / PUB:(DE-HGF)15},
      eprint       = {1409.0832},
      howpublished = {arXiv:1409.0832},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1409.0832;\%\%$},
      pubmed       = {pmid:26041974},
      url          = {https://bib-pubdb1.desy.de/record/187268},
}