000152708 001__ 152708
000152708 005__ 20210406095354.0
000152708 037__ $$aDESY-2013-00285
000152708 0881_ $$aCMS-SUS-12-024 ; CERN-PH-EP-2013-076
000152708 088__ $$2CMS$$aCMS-SUS-12-024
000152708 088__ $$2CERN$$aCERN-PH-EP-2013-076
000152708 1001_ $$0P:(DE-HGF)0$$aCMS Collaboration$$b0$$eCollaboration author
000152708 245__ $$aSearch for gluino mediated bottom- and top-squark production in multijet final states in pp collisions at 8 TeV
000152708 260__ $$c2013
000152708 3367_ $$0PUB:(DE-HGF)25$$2PUB:(DE-HGF)$$aPreprint$$bpreprint$$mpreprint$$s1373372548_14077
000152708 3367_ $$2DRIVER$$apreprint
000152708 3367_ $$2BibTeX$$aARTICLE
000152708 3367_ $$028$$2EndNote$$aElectronic Article
000152708 3367_ $$0PUB:(DE-HGF)15$$2PUB:(DE-HGF)$$aInternal Report$$mintrep
000152708 500__ $$aSubmitted to Phys. Lett. B
000152708 520__ $$aA search for supersymmetry is presented based on events with large missing transverse energy, no isolated electron or muon, and at least three jets, with one or more identified as a bottom-quark jet. A simultaneous examination is performed of the numbers of events in exclusive bins of the scalar sum of jet transverse momentum values, missing transverse energy, and bottom-quark jet multiplicity. The sample, corresponding to an integrated luminosity of 19.4 inverse femtobarns, consists of proton-proton collision data recorded at a center-of-mass energy of 8 TeV with the CMS detector at the LHC in 2012. The observed numbers of events are found to be consistent with the standard model expectation, which is evaluated with control samples in data. The results are interpreted in the context of two simplified supersymmetric scenarios in which gluino pair production is followed by the decay of each gluino to an undetected lightest supersymmetric particle and either a bottom or top quark-antiquark pair, characteristic of gluino mediated bottom- or top-squark production. Using the production cross section calculated to next-to-leading-order plus next-to-leading-logarithm accuracy, and in the limit of a massless lightest supersymmetric particle, we exclude gluinos with masses below 1170 GeV and 1020 GeV for the two scenarios, respectively.
000152708 536__ $$0G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405$$aExperiments at LHC (CMS) (POF2-512)$$cPOF2-512$$fPOF II$$x0
000152708 588__ $$aDataset connected to
000152708 693__ $$0EXP:(DE-H253)LHC-Exp-CMS-20150101$$1EXP:(DE-588)4398783-7$$5EXP:(DE-H253)LHC-Exp-CMS-20150101$$aLHC$$eLHC: CMS$$x0
000152708 909CO $$ooai:bib-pubdb1.desy.de:152708$$pVDB
000152708 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-HGF)0$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000152708 9131_ $$0G:(DE-HGF)POF2-512$$1G:(DE-HGF)POF2-510$$2G:(DE-HGF)POF2-500$$3G:(DE-HGF)POF2$$4G:(DE-HGF)POF$$9G:(DE-H253)POF2-LHC-Exp.-(CMS)-20130405$$aDE-H253CMS$$bStruktur der Materie$$lElementarteilchenphysik$$vLHC$$x0
000152708 9141_ $$y2013
000152708 9201_ $$0I:(DE-H253)CMS-20120731$$kCMS$$lLHC/CMS Experiment$$x0
000152708 980__ $$apreprint
000152708 980__ $$aVDB
000152708 980__ $$aUNRESTRICTED
000152708 980__ $$aintrep
000152708 980__ $$aI:(DE-H253)CMS-20120731