27 research outputs found

    Diffractive dijets with a leading anti-proton in anti-p p collisions at S**(1/2) = 1800-GeV

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    Search for second and third generation leptoquarks including production via technicolor interactions in p anti-p collisions at s**(1/2) = 1.8-TeV

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    We report the results of a search for second and third generation leptoquarks using 88 pb1{pb}^{-1} of data recorded by the Collider Detector at Fermilab. Color triplet technipions, which play the role of scalar leptoquarks, are investigated due to their potential production in decays of strongly coupled color octet technirhos. Events with a signature of two heavy flavor jets and missing energy may indicate the decay of a second (third) generation leptoquark to a charm (bottom) quark and a neutrino. As the data is found to be consistent with Standard Model expectations, mass limits are determined

    Search for scalar top quark production in anti-p p collisions at S**(1/2) = 1.8-TeV

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    We have searched for direct production of scalar top quarks at the Collider Detector at Fermilab in 88 pb-1 of p anti-p collisions at s**(1/2) = 1.8 TeV. We assume the scalar top quark decays into either a bottom quark and a chargino or a bottom quark, a lepton, and a scalar neutrino. The event signature for both decay scenarios is a lepton, missing transverse energy, and at least two b-quark jets. For a chargino mass of 90 GeV/c2 and scalar neutrino masses of at least 40 GeV/c2, we find no evidence for scalar top production and present upper limits on the production cross section in both decay scenarios.We have searched for direct production of scalar top quarks at the Collider Detector at Fermilab in 88 pb-1 of p anti-p collisions at s**(1/2) = 1.8 TeV. We assume the scalar top quark decays into either a bottom quark and a chargino or a bottom quark, a lepton, and a scalar neutrino. The event signature for both decay scenarios is a lepton, missing transverse energy, and at least two b-quark jets. For a chargino mass of 90 GeV/c2 and scalar neutrino masses of at least 40 GeV/c2, we find no evidence for scalar top production and present upper limits on the production cross section in both decay scenarios

    Search for scalar top and scalar bottom quarks in p anti-p collisions at S**(1/2) = 1.8-TeV

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    We have searched for direct pair production of scalar top and scalar bottom quarks in 88 pb1^{-1} of ppˉp\bar{p} collisions at s=1.8\sqrt{s}=1.8 TeV with the CDF detector. We looked for events with a pair of heavy flavor jets and missing energy, consistent with scalar top quark decays to a charm quark and a neutralino, or scalar bottom quark decays to a bottom quark and a neutralino. The numbers of events that pass our selection for each process show no deviation from Standard Model expectations. We compare our results to next-to-leading order calculations for the scalar quark production cross sections to exclude regions in scalar quark-neutralino parameter space

    Search for the flavor changing neutral current decays B+ ---> muon+ muon- K+ and B0 ---> muon+ muon- K*0

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    We report on a search for the flavor-changing neutral current decays B^+ -> mu^+ mu^- K^+ and B^0 -> mu^+ mu^- K^{*0} using 88 pb^{-1} of data from p-pbar collisions at \sqrt{s}=1.8 TeV, collected with the Collider Detector at Fermilab. Finding no evidence for these decays, we set upper limits on the branching fractions B(B^+ -> mu^+ mu^- K^+) mu^+ mu^-K^{*0}) < 4.0x10^{-6} at the 90% confidence level

    Observation of orbitally excited B mesons in p anti-p collisions at S**(1/2) = 1.8-TeV

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    A Measurement of sin 2 Beta from B ---> J / psi K0(S) with the CDF detector

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    This paper reports an updated measurement of the Standard Model CP violation parameter sin2β\sin2\beta using the CDF Detector at Fermilab. The entire Run I data sample of 110 pb1^{-1} of proton antiproton collisions at s=1.8TeV\sqrt{s}=1.8 TeV is used to identify a signal sample of 400\sim 400 BJ/ψKS0B \to J/\psi K^0_S events, where J/ψμ+μJ/\psi \to \mu^+\mu^- and KS0π+πK_S^0 \to \pi^+\pi^-. The flavor of the neutral B meson is identified at the time of production by combining information from three tagging algorithms: a same-side tag, a jet-charge tag, and a soft-lepton tag. A maximum likelihood fitting method is used to determine sin2β=0.79+0.410.44\sin2\beta = 0.79 {+0.41\atop-0.44}(stat+syst). This value of sin2β\sin 2 \beta is consistent with the Standard Model prediction, based upon existing measurements, of a large positive CP violating asymmetry in this decay mode

    Search for the decay B/s --> mu+ mu- Phi in p anti-p collisions at s**(1/2) = 1.8-TeV

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    Dijet production by double pomeron exchange at the Fermilab Tevatron

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    A Study of B0 ---> J / psi K(*)0 pi+ pi- decays with the collider detector at Fermilab

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    We report a study of the decays B0 -> J/psi K(*)0 pi+ pi-, which involve the creation of a u u-bar or d d-bar quark pair in addition to a b-bar -> c-bar(c s-bar) decay. The data sample consists of 110 1/pb of p p-bar collisions at sqrt{s} = 1.8 TeV collected by the CDF detector at the Fermilab Tevatron collider during 1992-1995. We measure the branching ratios to be BR(B0 -> J/psi K*0 pi+ pi-) = (8.0 +- 2.2 +- 1.5) * 10^{-4} and BR(B0 -> J/psi K0 pi+ pi-) = (1.1 +- 0.4 +- 0.2) * 10^{-3}. Contributions to these decays are seen from psi(2S) K(*)0, J/psi K0 rho0, J/psi K*+ pi-, and J/psi K1(1270)
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