9 research outputs found

    A High statistics study of states containing heavy quarks using the wide band photon beam and the E-687 multiparticle spectrometer.

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    The spectrometer used in Fermilab experiment 687 to study the photoproduction and decay of charm particles will be upgraded to enable it to accumulate 10**6 fully reconstructed charm particles. The physics will involve high precision studies of the D semileptonic decays, QCD studies of double D events, a measurement of the absolute branching fraction for the D0, searches for the D0 mixing, CP violation, rare and forbidden decays, fully leptonic decays of the D+ and a systematic investigation of charm baryons and their lifetimes

    Search for CP violation in charm meson decay

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    We report the results of a search for CP-violating decay rate asymmetries (ACP) in the charm decay modes D+\u2192K-K+pi+, D+\u2192K\uaf*0K+, D+\u2192phi pi+, and D0\u2192K+K-. Our measurements are all consistent with zero asymmetry: ACP(KKpi)=-0.031\ub10.068, ACP(K*K)=-0.12\ub10.13, ACP(phi pi)=0.066\ub10.086, and ACP(KK)=0.024\ub10.084. The data were accumulated by the Fermilab high energy photoproduction experiment E68

    ANALYSIS OF THE DECAY MODE D+ -> anti(K*0) MU+NU

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    Fermilab high-energy photoproduction experiment E687 provides a high statistics sample of the decay mode D+ \u2192 anti(K 170) mu+nu (charge conjugates are implied). Our analysis yields a branching ratio of Gamma (D+ \u2192 anti(K 170)mu+\u3bd)/Gamma(D+ \u2192 K 12pi+pi+) = 0.56\ub10.04\ub10.06. The ratios of the form factors governing the decay are measured to be R\u3bd = 1.74 \ub10.27\ub10.28 and R2 = 0.78\ub10.18\ub10.10, implying a polarization of Gammal/Gammat = 1.20\ub10.13 \ub10.13 for the electron decay. Finally, we report new limits on the decay modes D+ \u2192 K-pi+mu+nu (nonresonent) and D+ \u2192 anti(K 170) pi0 mu+nu

    Semileptonic charmed meson decays.

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    Results on the semileptonic channels: Do→K+μ−ν+c.c. and D+→K∗oμ+ν+c.c., photoproduced in the E687 experiment at Fermilab, are presented. A preliminary measurement of Γ(Do→K∗−μν)/Γ(D+→K∗oμν) is also discussed
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