97 research outputs found

    First Measurement of the Branching Fraction of e^+e^- --> B0B0bar

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    We report the first measurement of the absolute branching fraction e^+e^- --> B0B0bar at the Upsilon(4S) resonance using data collected with the BABAR detector at the PEP-II asymmetric-energy e^+e^- storage ring. The analysis is performed with partial reconstruction of the decay B0bar --> D^{*+}\ell^{-} \bar{\nu}_{\ell},wherethepresenceofasignaldecayisdeterminedusingonlytheleptonandthesoftpionfromtheD∗decay.Byreconstructingeventswithoneortwosignaldecaysweobtainapreliminaryresultofe+e−−−>B0B0bar=0.486±0.010(stat.)±0.009(sys.), where the presence of a signal decay is determined using only the lepton and the soft pion from the D^{*} decay. By reconstructing events with one or two signal decays we obtain a preliminary result of e^+e^- --> B0B0bar = 0.486 \pm 0.010(stat.) \pm 0.009(sys.). Our result does not depend on branching fractions of the B0bar and the D^{*+} decay chains, on the individual simulated reconstruction efficiencies, on the ratio of the charged and neutral B meson lifetimes, or on the assumption of isospin symmetry.Comment: Latex, 5 pages, 2 figures, proceedings to the DPF 2004, 26 August-31 August 2004, Riverside, CA, US

    Search For New Physics at BABAR

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    Using a full BABAR data sample of 426 fb−1fb^{-1}, we present improved measurements of the ratio R(D(∗))=B(Bˉ→D(∗)τ−νˉτ)/{\cal{R}}(D^{(*)}) = {\cal{B}} (\bar{B} \to D^{(*)}\tau^{-}\bar{\nu}_{\tau})/ B(Bˉ→D(∗)ℓℓ−νˉℓ){\cal{B}} (\bar{B} \to D^{(*)}\ell_{\ell}^{-}\bar{\nu}_{\ell}), where ℓ\ell is either electron or muon. We measure R(D)=0.440±0.058±0.042{\cal{R}}(D) = 0.440 \pm 0.058 \pm 0.042 and R(D∗)=0.332±0.024±0.018{\cal{R}}(D^*) = 0.332 \pm 0.024 \pm 0.018. These ratios exceed the Standard Model predictions by 2.0σ2.0\sigma and 2.7σ2.7\sigma, respectively. The results disagree with the Standard Model predictions at the level of 3.4σ3.4\sigma. The ratios are sensitive to new physics contributions in the form of a charged Higgs boson. However, the access cannot be explained by a charged Higgs boson in the type II two-Higgs-doublet model.Comment: Contributed to the Proceedings of Hadron Collider Physics Symposium 2012, Kyoto, Japan, November 12-16 201

    Measurements of |V_{cb}| and |V_{ub}| at BABAR

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    We report on new measurements of the Cabibbo-Kobayashi-Maskawa matrix elements |V_{cb}| and |V_{ub}| with inclusive and exclusive semileptonic B decays, highlighting the recent precision measurements with the BABAR detector at the PEP-II asymmetric-energy B Factory at SLAC.Comment: Comments : Latex, 4 pages. Talk given at PANIC05: The Particles and Nuclei International Conference, October 24-28, 2005 Santa Fe, USA. Proceedings to appear in the American Institute of Physic

    Hot Topics From BABAR Experiment

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    We search for a new light non-Standard Model CP-odd Higgs boson, A0A^0, decaying to τ+τ−\tau^+\tau^-, μ+μ−\mu^+\mu^-, and invisible in radiative decays of the Υ(2S)\Upsilon(2S) and Υ(3S)\Upsilon(3S). We search for the light scalar particle produced in single-photon decays of the Υ(3S)\Upsilon(3S) resonance through the process Υ(3S)→γA0,A0→\Upsilon(3S) \to \gamma A^0, A^0 \to invisible. We also search for evidence of an undetectable Υ(1S)\Upsilon(1S) decay recoiling against the dipion system. The data samples contain 99×106Υ(2S)99 \times 10^6 \Upsilon(2S) and 122×106Υ(3S)122 \times 10^6 \Upsilon(3S) decays collected by the \babar\ detector at the SLAC PEP-II BB factory.Comment: Contributed to the Proceedings of 16th International Seminar on High Energy Physics QUARKS-2010, Kolomna, Russia, 6-12 June, 201

    Charm Decays and Spectroscopy at BABAR

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    We present searches for rare charm decays of the form Xc+→h±ℓ∓ℓ(′)+X_c^+ \to h^{\pm} \ell^{\mp} \ell^{(')^+}, where Xc+X_c^+ is a charm hadron either D+D^+, Ds+D_s^+, or Λc+\Lambda_c^+, and ℓ(′)±\ell^{(')^{\pm}} is an electron or muon. These modes are based on 384 fb−1fb^{-1} of e+e−e^+ e^- annihilation data collected at the Υ(4S)\Upsilon(4S) resonance with the BABAR detector at the SLAC National Accelerator Laboratory. We also present the flavor-changing neutral-current decays D0→e+e−D^0 \to e^+e^-, D0→μ+μ−D^0 \to \mu^+ \mu^-, and D0→e±μ∓D^0 \to e^{\pm} \mu^{\mp} that corresponds to an integrated luminosity of 468 fb−1fb^{-1} of data. The decay D0→e+μ−D^0 \to e^+ \mu^- is further lepton-flavor violating, and thus occur only through very slow neutrino mixing. These decays constitute sensitive probes for possible new-physics contribution. We report new limits on the branching fractions of these decays.Comment: Contributed to the Proceedings of 36th International Conference on High Energy Physics, July 4-11, 2012, Melbourne, Australia. This work was supported by the U.S. Department of Energy under grant No. DE-FG02-96ER-4097
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