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      First Search for Multijet Resonances in \(\sqrt{s} = 1.96\) TeV \( p\bar{p}\) Collisions

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          Abstract

          We present the first model independent search for three-jet hadronic resonances within multijet events in \(\sqrt{s} = 1.96\) TeV \(p\bar{p}\) collisions at the Fermilab Tevatron using the CDF II detector. Pair production of supersymmetric gluinos and squarks with hadronic R-parity violating decays is employed as an example of a new physics benchmark for this signature. Selection criteria based on the kinematic properties of an ensemble of jet combinations within each event help to extract signal from copious QCD background. Our background estimates include all-hadronic \(t\bar{t}\) decays that have a signature similar to the signal. No significant excess outside the top quark mass window is observed in data with an integrated luminosity of 3.2 fb\(^{-1}\). We place 95% confidence level limits on the production cross section \(\sigma(p \bar{p} \rightarrow XX^{'}) \times \rm{BR}\)(\(\widetilde{g}\widetilde{g}\)$ \rightarrow 3 {\rm jet}+3 {\rm jet})\( where \)X, X' = \widetilde{g}, \widetilde{q}\(, or \)\widetilde{\bar{q}}\(, with \)\widetilde{q}\(, \)\widetilde{\bar{q}} \rightarrow \widetilde{g}\( + jet, as a function of gluino mass, in the range of 77 GeV/\)c^2\( to 240 GeV/\)c^2$.

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          Matching NLO QCD and parton showers in heavy flavour production

          We apply the MC@NLO approach to the process of heavy flavour hadroproduction. MC@NLO is a method for matching next-to-leading order (NLO) QCD calculations and parton shower Monte Carlo (MC) simulations, with the following features: fully exclusive events are generated, with hadronisation according to the MC model; total rates are accurate to NLO; NLO results for distributions are recovered upon expansion in \(\as\); hard emissions are treated as in NLO computations while soft/collinear emissions are handled by the MC simulation, with the same logarithmic accuracy as the MC; matching between the hard and soft regions is smooth, and no intermediate integration steps are necessary. The method was applied previously to the hadroproduction of gauge boson pairs, which at NLO involves only initial-state QCD radiation and a unique colour structure. In heavy flavour production, it is necessary to include contributions from final-state QCD radiation and different colour flows. We present illustrative results on top and bottom production at the Tevatron and LHC.
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            Author and article information

            Journal
            13 May 2011
            2011-06-24
            Article
            10.1103/PhysRevLett.107.042001
            1105.2815
            df0c36de-2da4-483b-8a9a-89cd57663bcb

            http://creativecommons.org/licenses/publicdomain/

            History
            Custom metadata
            FERMILAB-PUB-11-220-E-PPD
            Phys.Rev.Lett.107:042001,2011
            7 pages, 3 figures, accepted by Phys. Rev. Lett
            hep-ex

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