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002217927 003__ SzGeCERN
002217927 005__ 20210917045343.0
002217927 0248_ $$aoai:cds.cern.ch:2217927$$pcerncds:CERN$$pINIS$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002217927 0247_ $$2DOI$$a10.22323/1.276.0145
002217927 035__ $$9arXiv$$aoai:arXiv.org:1609.07445
002217927 035__ $$9Inspire$$a1487911
002217927 037__ $$9arXiv$$aarXiv:1609.07445$$chep-ex
002217927 037__ $$9arXiv:reportnumber$$aCMS-CR-2016-216
002217927 041__ $$aeng
002217927 100__ $$aSakuma, Tai$$iINSPIRE-00122640$$mtai.sakuma@cern.ch$$uBristol U.$$vUniversity of Bristol (UK)
002217927 245__ $$aSquark/gluino searches in hadronic channels with CMS
002217927 269__ $$aGeneva$$bCERN$$c05 Sep 2016
002217927 260__ $$bSISSA$$c2017-03-21
002217927 300__ $$a10 p
002217927 500__ $$9arXiv$$aProceedings for 4th Conference on Large Hadron Collider Physics 2016
(LHCP 2016), Lund, Sweden
002217927 520__ $$aThese proceedings summarize the results of four analyses which searched for squarks and gluinos in hadronic final states with missing transverse momentum in 2.3~fb$^{-1}$ of data in proton-proton collisions at $\sqrt{s}=13$~TeV collected in the year 2015 with the CMS detector at the CERN LHC. Each analysis is characterized by a different kinematic variable that is sensitive to the presence of invisible particles, e.g., $M_\text{T2}$, $\alpha_{\text{T}}$, and \textit{razor} variables. We observed no significant deviation from the standard model prediction and placed limits on the production cross sections and the masses of squarks and gluinos in simplified models of supersymmetric models. The limits are significantly extended from the previous results.
002217927 520__ $$9arXiv$$aThese proceedings summarize the results of four analyses which searched for squarks and gluinos in hadronic final states with missing transverse momentum in 2.3 fb$^{-1}$ of data in proton-proton collisions at $\sqrt{s}=13$ TeV collected in the year 2015 with the CMS detector at the CERN LHC. Each analysis is characterized by a different kinematic variable that is sensitive to the presence of invisible particles, e.g., $M_\text{T2}$, $\alpha_{\text{T}}$, and razor variables. We observed no significant deviation from the standard model prediction and placed limits on the production cross sections and the masses of squarks and gluinos in simplified models of supersymmetric models. The limits are significantly extended from the previous results.
002217927 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002217927 540__ $$3Preprint$$aCC-BY-4.0
002217927 595__ $$aautomerged
002217927 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
002217927 6531_ $$9CMS$$aSUSY
002217927 690C_ $$aINTNOTE
002217927 690C_ $$aCERN
002217927 690C_ $$aPUBLCMS
002217927 693__ $$aCERN LHC$$eCMS
002217927 695__ $$9LANL EDS$$ahep-ex
002217927 710__ $$5PH
002217927 710__ $$gCMS Collaboration
002217927 773__ $$c145$$pPoS$$vLHCP2016$$wC16-06-13$$y2017
002217927 8564_ $$uhttps://pos.sissa.it/archive/conferences/276/145/LHCP2016_145.pdf$$yPoS server
002217927 8564_ $$81244554$$s785989$$uhttps://cds.cern.ch/record/2217927/files/CR2016_216.pdf
002217927 8564_ $$81292848$$s749478$$uhttps://cds.cern.ch/record/2217927/files/arXiv:1609.07445.pdf
002217927 8564_ $$81292842$$s60894$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-002_Figure_006.png$$y00002 The observed number of the events and the SM background predictions in each of the 72 bins in the search region of the analysis in Ref.~\cite{Khachatryan:2016kdk}.
002217927 8564_ $$81292843$$s82303$$uhttps://cds.cern.ch/record/2217927/files/T1tttt_Moriond.png$$y00014 : The limits on the \PSGcz-\PSg mass plane for T1tttt placed by the four analyses summarized in these proceedings \cite{Khachatryan:2016kdk,Khachatryan:2016xvy,CMS-PAS-SUS-15-004,CMS-PAS-SUS-15-005,CMS-PAS-SUS-16-004}, four other analyses with the data collected during the same period \cite{CMS-PAS-SUS-15-006,Khachatryan:2016uwr,Khachatryan:2016kod,CMS-PAS-SUS-16-003}, and one analysis with Run~1 data \cite{CMS:2014dpa}. The solid lines show the observed limits, and dashed lines show the e
002217927 8564_ $$81292844$$s51614$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-003_Figure-aux_003.png$$y00004 : \textit{(top)} The boundaries of the \HT and \MTtwo bins for $\njet \ge 2$ and \textit{(bottom)} the boundaries of the jet \pt bins for $\njet = 1$ in Ref.~\cite{Khachatryan:2016xvy}.
002217927 8564_ $$81292845$$s4703$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-003_Figure-aux_004.png$$y00005 : Caption not extracted
002217927 8564_ $$81292846$$s62265$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-002_Figure-aux_001.png$$y00001 : Background composition of the SM processes in the bins of \njet and \nb evaluated in simulation in the analysis in Ref.~\cite{Khachatryan:2016kdk}.
002217927 8564_ $$81292847$$s67059$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-003_Figure_008-b.png$$y00006 The observed number of the events and the SM background predictions in the \njet, \nb, and \MTtwo bins in one of the \HT bins in the search region of the analysis in Ref.~\cite{Khachatryan:2016xvy}.
002217927 8564_ $$81292849$$s8429$$uhttps://cds.cern.ch/record/2217927/files/CMS-PAS-SUS-15-004_Figure_002-a.png$$y00007 The sidebands and the signal region on the $M_\textrm{T}^\textrm{R}$-$R^2$ plane in the multijet category in Ref.~\cite{CMS-PAS-SUS-15-004}
002217927 8564_ $$81292850$$s98610$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-003_Figure_011-c.png$$y00013 : The limit on the production cross section of squark pairs and on the masses on the \PSGcz-\PSQ mass plane in T2qq for the case in which both chiral states of all light-flavored squark have the same mass and the case in which one chiral state of one light-flavored squark enters the model \cite{Khachatryan:2016xvy}.
002217927 8564_ $$81292851$$s65039$$uhttps://cds.cern.ch/record/2217927/files/T1bbbb_Moriond.png$$y00015 : The limits on the \PSGcz-\PSg mass plane for T1bbbb placed by the four analyses summarized in these proceedings \cite{Khachatryan:2016kdk,Khachatryan:2016xvy,CMS-PAS-SUS-15-004,CMS-PAS-SUS-15-005} and one analysis with Run~1 data \cite{CMS-PAS-SUS-14-011}.
002217927 8564_ $$81292852$$s30033$$uhttps://cds.cern.ch/record/2217927/files/CMS-PAS-SUS-15-005_Figure_002-a.png$$y00008 The distribution of \alphat in the data and estimates of the contributions from the QCD multijet events and the other SM events \cite{CMS-PAS-SUS-15-005}.
002217927 8564_ $$81292853$$s60947$$uhttps://cds.cern.ch/record/2217927/files/T1qqqq_Moriond.png$$y00016 : The limits on the \PSGcz-\PSg mass plane for T1qqqq placed by the four analyses summarized in these proceedings \cite{Khachatryan:2016kdk,Khachatryan:2016xvy,CMS-PAS-SUS-15-004,CMS-PAS-SUS-15-005} and one analysis with Run~1 data \cite{Khachatryan:2015vra}.
002217927 8564_ $$81292854$$s33821$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-003_Figure_001.png$$y00003 : Distributions of \MTtwo in simulated events for the SM background processes and a signal process \cite{Khachatryan:2016xvy}.
002217927 8564_ $$81292855$$s11429$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-002_Figure_002.png$$y00000 : A schematic diagram of the categories used in Ref.~\cite{Khachatryan:2016kdk}, i.e., bins in \HT and \MHT. Events in each bin in the diagram are further binned in \njet and \nb.
002217927 8564_ $$81292856$$s2641$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-003_Figure_009-f.png$$y00009 Diagrams for the gluino pair and squark pair productions in simplified models: T2qq \textit{(top left)}, T1tttt \textit{(top right)}, T1bbbb \textit{(bottom left)}, T1qqqq \textit{(bottom right)}.
002217927 8564_ $$81292857$$s3657$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-002_Figure_001-b.png$$y00010 Diagrams for the gluino pair and squark pair productions in simplified models: T2qq \textit{(top left)}, T1tttt \textit{(top right)}, T1bbbb \textit{(bottom left)}, T1qqqq \textit{(bottom right)}.
002217927 8564_ $$81292858$$s3688$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-002_Figure_001-c.png$$y00012 Diagrams for the gluino pair and squark pair productions in simplified models: T2qq \textit{(top left)}, T1tttt \textit{(top right)}, T1bbbb \textit{(bottom left)}, T1qqqq \textit{(bottom right)}.
002217927 8564_ $$81292859$$s3682$$uhttps://cds.cern.ch/record/2217927/files/CMS-SUS-15-002_Figure_001-a.png$$y00011 Diagrams for the gluino pair and squark pair productions in simplified models: T2qq \textit{(top left)}, T1tttt \textit{(top right)}, T1bbbb \textit{(bottom left)}, T1qqqq \textit{(bottom right)}.
002217927 8564_ $$81302595$$s724175$$uhttps://cds.cern.ch/record/2217927/files/PoS(LHCP2016)145.pdf$$yFulltext
002217927 8564_ $$81512169$$s749478$$uhttps://cds.cern.ch/record/2217927/files/1609.07445.pdf$$yFulltext
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