2 research outputs found

    First Measurement of the \lowercase{\ttbar} Differential Cross Section \lowercase{d\sigma/d}M_{\lowercase{{t\overline{t}}}} in \lowercase{\ppbar} Collisions at \sqrt{\lowercase{s}}=1.96 TeV

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    8 pages, 1 figureWe present a measurement of the \ttbar differential cross section with respect to the \ttbar invariant mass, dSigma/dMttbar, in \ppbar collisions at s=1.96\sqrt{s}=1.96 TeV using an integrated luminosity of 2.7\invfb collected by the CDF II experiment. The \ttbar invariant mass spectrum is sensitive to a variety of exotic particles decaying into \ttbar pairs. The result is consistent with the standard model expectation, as modeled by \texttt{PYTHIA} with \texttt{CTEQ5L} parton distribution functions.We present a measurement of the tt̅ differential cross section with respect to the tt̅ invariant mass, dσ/dMtt̅ , in pp̅ collisions at √s=1.96  TeV using an integrated luminosity of 2.7  fb-1 collected by the CDF II experiment. The tt̅ invariant mass spectrum is sensitive to a variety of exotic particles decaying into tt̅ pairs. The result is consistent with the standard model expectation, as modeled by PYTHIA with CTEQ5L parton distribution functions.Peer reviewe

    Search for the Neutral Current Top Quark Decay t-->Zc Using the Ratio of Z-Boson + 4 Jets to W-Boson + 4 Jets Production

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    We have used the Collider Detector at Fermilab (CDF II) to search for the flavor-changing neutral-current (FCNC) top quark decay {t\goes Zc} using a technique employing ratios of WW and ZZ production, measured in \ppbar data corresponding to an integrated luminosity of 1.52 fb−1fb^{-1}. The analysis uses a comparison of two decay chains, {p\bar{p}\goes t\bar{t}\goes WbWb\goes\ell\nu bjjb} and {p\bar{p}\goes t\bar{t}\goes ZcWb\goes\ell\ell cjjb}, to cancel systematic uncertainties in acceptance, efficiency, and luminosity. We validate the modeling of acceptance and efficiency for lepton identification over the multi-year dataset using another ratio of WW and ZZ production, in this case the observed ratio of inclusive production of WW to ZZ bosons. To improve the discrimination against standard model backgrounds to top quark decays, we calculate the top quark mass for each event with two leptons and four jets assuming it is a ttˉt\bar{t} event with one of the top quarks decaying to ZcZc. For additional background discrimination we require at least one jet to be identified as originating from a bb-quark. No significant signal is found and we set an upper limit on the FCNC branching ratio Br({t\goes Zc}) using a likelihood constructed from the ℓℓcjjb{\ell\ell cjjb} top quark mass distribution and the number of ℓνbjjb{\ell\nu bjjb} events. Limits are set as a function of the helicity of the ZZ boson produced in the FCNC decay. For 100% longitudinally polarized ZZ bosons we find limits of 8.3% and 9.3% (95% C.L.) depending on the assumptions regarding the theoretical top quark pair production cross-section
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