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Evidence for the decay D0-->K(-)pi(+)pi(-)e(+)nu(e)
Authors:Artuso M  Blusk S  Butt J  Li J  Menaa N  Mountain R  Nisar S  Randrianarivony K  Sia R  Skwarnicki T  Stone S  Wang J C  Zhang K  Bonvicini G  Cinabro D  Dubrovin M  Lincoln A  Asner D M  Edwards K W  Naik P  Briere R A  Ferguson T  Tatishvili G  Vogel H  Watkins M E  Rosner J L  Adam N E  Alexander J P  Cassel D G  Duboscq J E  Ehrlich R  Fields L  Galik R S  Gibbons L  Gray R  Gray S W  Hartill D L  Heltsley B K  Hertz D  Jones C D  Kandaswamy J  Kreinick D L  Kuznetsov V E  Mahlke-Krüger H  Mohapatra D  Onyisi P U E  Patterson J R  Peterson D  Pivarski J  Riley D  Ryd A  Sadoff A J  Schwarthoff H  Shi X  Stroiney S  Sun W M  Wilksen T
Institution:Syracuse University, Syracuse, NY 13244, USA.
Abstract:Using a 281 pb{-1} data sample collected at the psi(3770) with the CLEO-c detector, we present the first absolute branching fraction measurement of the decay D0-->K(-)pi(+)pi(-)e(+)nu(e) at a statistical significance of about 4.0 standard deviations. We find 10 candidates consistent with the decay D0-->K(-)pi(+)pi(-)e(+)nu(e). The probability that a background fluctuation accounts for this signal is less than 4.1 x 10{-5}. We find B(D0-->K(-)pi(+)pi(-)e(+)nu(e)) = 2.8{-1.1}{+1.4}(stat)+/-0.3(syst)]x10{-4}. By restricting the invariant mass of the hadronic system to be consistent with K1(1270), we obtain the product of branching fractions B(D{0}-->K{1}{-}(1270)e{+}nu{e})xB(K1-(1270)-->K{-}pi{+}pi{-})=2.5{-1.0}{+1.3}(stat)+/-0.2(syst)]x10{-4}. Using B(K1-(1270)-->K{-}pi{+}pi{-})=(33+/-3)%, we obtain B(D{0}-->K{1}{-}(1270)e{+}nu{e})=7.6{-3.0}{+4.1}(stat)+/-0.6(syst)+/-0.7]x10{-4}. The last error accounts for the uncertainties in the measured K1-(1270)-->K{-}pi{+}pi{-} branching fractions.
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