2008
DOI: 10.2172/938891
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Search for super symmetry at the Tevatron using the trilepton signature

Abstract: This dissertation describes a search for the associated production of the supersymmetric particles, the chargino and the neutralino, through their R-parity conserving decays to three leptons and missing energy. This search is carried out using the data collected at the CDF experiment at the Tevatron √ s = 1.96 TeV pp collider at Fermilab. The results are obtained by combining five independent channels with varying signal to background ratio. Overall, a total of 6.4 ± 1.1 background events from standard model p… Show more

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Cited by 6 publications
(13 citation statements)
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“…This is populated mainly by Drell-Yan production, and its acceptance should be dominated by the per-lepton acceptance. (10) The CDF analysis includes two types of electrons and two types of muons, referred to separately as tight and loose to represent more and less stringent ID requirements, respectively [36]. We find that PGS leptons are not refined enough to make this differentiation.…”
Section: A2 Trileptonsmentioning
confidence: 95%
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“…This is populated mainly by Drell-Yan production, and its acceptance should be dominated by the per-lepton acceptance. (10) The CDF analysis includes two types of electrons and two types of muons, referred to separately as tight and loose to represent more and less stringent ID requirements, respectively [36]. We find that PGS leptons are not refined enough to make this differentiation.…”
Section: A2 Trileptonsmentioning
confidence: 95%
“…For a full description of the analysis, we refer the reader to Refs. [16,17] and especially the thesis [36]. The CDF trilepton search selects events from two categories: three leptons, lll, or two leptons and one isolated track llT (7) .…”
Section: Trileptonsmentioning
confidence: 99%
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“…This happens with an efficiency of 1 antiproton per 10000 protons [19]. This production mechanism leads to a particle beam with a wide range of momentum.…”
Section: The Antiproton Sourcementioning
confidence: 99%
“…At the Tevatron the time between two bunch crossings and therefore theoretically two events is 392 ns, or a frequency of 2.5 MHz [19]. To store every single one of these events would not just be a huge challenge for the electronics but also would not be useful for analyses since only a fraction of the events are physically interesting.…”
Section: Trigger Systemmentioning
confidence: 99%