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@ARTICLE{Chatrchyan:155997,
      author       = {Chatrchyan, Serguei and others},
      title        = {{S}earch for gluino mediated bottom- and top-squark
                      production in multijet final states in pp collisions at 8
                      {T}e{V}},
      journal      = {Physics letters / B},
      volume       = {725},
      number       = {4-5},
      issn         = {0370-2693},
      address      = {Amsterdam},
      publisher    = {North-Holland Publ.},
      reportid     = {DESY-2014-00051, arXiv:1305.2390. CMS-SUS-12-024.
                      CERN-PH-EP-2013-076},
      pages        = {243 - 270},
      year         = {2013},
      note         = {© 2013 CERN},
      abstract     = {A search for supersymmetry is presented based on events
                      with large missing transverse energy, no isolated electron
                      or muon, and at least three jets with one or more identified
                      as a bottom-quark jet. A simultaneous examination is
                      performed of the numbers of events in exclusive bins of the
                      scalar sum of jet transverse momentum values, missing
                      transverse energy, and bottom-quark jet multiplicity. The
                      sample, corresponding to an integrated luminosity of 19.4
                      inverse femtobarns, consists of proton-proton collision data
                      recorded at a center-of-mass energy of 8 TeV with the CMS
                      detector at the LHC in 2012. The observed numbers of events
                      are found to be consistent with the standard model
                      expectation, which is evaluated with control samples in
                      data. The results are interpreted in the context of two
                      simplified supersymmetric scenarios in which gluino pair
                      production is followed by the decay of each gluino to an
                      undetected lightest supersymmetric particle and either a
                      bottom or top quark-antiquark pair, characteristic of gluino
                      mediated bottom- or top-squark production. Using the
                      production cross section calculated to next-to-leading-order
                      plus next-to-leading-logarithm accuracy, and in the limit of
                      a massless lightest supersymmetric particle, we exclude
                      gluinos with masses below 1170 GeV and 1020 GeV for the two
                      scenarios, respectively. Elsevier A search for supersymmetry
                      is presented based on events with large missing transverse
                      energy, no isolated electron or muon, and at least three
                      jets with one or more identified as a bottom-quark jet. A
                      simultaneous examination is performed of the numbers of
                      events in exclusive bins of the scalar sum of jet transverse
                      momentum values, missing transverse energy, and bottom-quark
                      jet multiplicity. The sample, corresponding to an integrated
                      luminosity of 19.4 $fb^-^1,$ consists of proton-proton
                      collision data recorded at a center-of-mass energy of 8 TeV
                      with the CMS detector at the LHC in 2012. The observed
                      numbers of events are found to be consistent with the
                      standard model expectation, which is evaluated with control
                      samples in data. The results are interpreted in the context
                      of two simplified supersymmetric scenarios in which gluino
                      pair production is followed by the decay of each gluino to
                      an undetected lightest supersymmetric particle and either a
                      bottom or top quark-antiquark pair, characteristic of gluino
                      mediated bottom- or top-squark production. Using the
                      production cross section calculated to next-to-leading-order
                      plus next-to-leading-logarithm accuracy, and in the limit of
                      a massless lightest supersymmetric particle, we exclude
                      gluinos with masses below 1170 GeV and 1020 GeV for the two
                      scenarios, respectively.},
      cin          = {CMS},
      ddc          = {530},
      cid          = {I:(DE-H253)CMS-20120731},
      pnm          = {Experiments at LHC (CMS) (POF2-512)},
      pid          = {G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405},
      experiment   = {EXP:(DE-H253)LHC-Exp-CMS-20150101},
      typ          = {PUB:(DE-HGF)16 / PUB:(DE-HGF)15},
      eprint       = {1305.2390},
      howpublished = {arXiv:1305.2390},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:1305.2390;\%\%$},
      doi          = {10.1016/j.physletb.2013.06.058},
      url          = {https://bib-pubdb1.desy.de/record/155997},
}