934,507 research outputs found

    Measurement of the B0Bˉ0B^0 -\bar{B}^0 mixing rate with B0(Bˉ0)Dπ±B^0(\bar{B}^0) \to D^{*\mp} \pi^{\pm} partial reconstruction

    Full text link
    We report a measurement of the B0Bˉ0B^0-\bar{B}^0 mixing parameter Δmd\Delta m_d based on a 29.1 fb1\rm 29.1~fb^{-1} sample of Υ(4S)\Upsilon (4S) resonance decays collected by the Belle detector at the KEKB asymmetric e+ee^+ e^- collider. We use events with a partially reconstructed B0(Bˉ0)Dπ±B^0(\bar{B}^0) \to D^{*\mp} \pi^{\pm} candidate and where the flavor of the accompanying BB meson is identified by the charge of the lepton from a B0(Bˉ0)X±νB^0(\bar{B}^0) \to X^{\mp} \ell^{\pm} \nu decay. The proper-time difference between the two BB mesons is determined from the distance between the two decay vertices. From a simultaneous fit to the proper-time distributions for the same-flavor (B0(Bˉ0)B^0(\bar{B}^0), ±\ell^{\pm}) and opposite-flavor (B0(Bˉ0)B^0(\bar{B}^0), \ell^{\mp}) event samples, we measure the mass difference between the two mass eigenstates of the neutral BB meson to be Δmd\Delta m_d= (0.509±0.017 (stat)±0.020 (syst)) ps1(0.509 \pm 0.017~(\rm stat) \pm 0.020~(\rm syst))~ps^{-1}.Comment: 16 pages, 14 figure

    B^0-\bar{B}^0 mixing with quenched lattice NRQCD

    Get PDF
    We present our recent results for the B-parameters, which parameterize the \Delta B=2 transition amplitudes. Calculations are made in quenched QCD at \beta=5.7, 5.9, and 6.1, using NRQCD for heavy quark and the O(a)O(a)-improved action for light quark. The operators are perturbatively renormalized including corrections of O(\alpha_s/am_Q). We examine scaling behavior of the B-parameters in detail, and discuss the systematic uncertainties using scatter of results with different analysis procedures adopted. As a result, we find B_{B_d}(m_b)=0.84(2)(8), B_{B_s}/B_{B_d}=1.017(10)(^{+4}_{-0}) and B_{S_s}(m_b)=0.87(1)(9)(^{+1}_{-0}) in the quenched approximation.Comment: Lattice 2000 (Heavy Quark Physics), 4 pages, 4 eps-figures, Latex, typo correcte

    Electroweak effects in the B0Bˉ0B^0-{\bar B}^0 mixing

    Full text link
    We compute analytically the complete electroweak two-loop corrections to the B0Bˉ0B^0-{\bar B}^0 mixing. These corrections fix the normalization of the electroweak coupling employed in the extraction of Vtd|V_{td}| and reduce the theoretical uncertainty due to higher order electroweak effects from several percent to a few parts in a thousand. If the LO result is expressed in terms of GμG_\mu or of the MSˉ\bar{MS} coupling g^(MZ)\hat{g}(M_Z), the two-loop corrections are O(1O(1%), the exact value depending on the mass of the Higgs boson. We discuss in detail the renormalization procedure and the scheme and scale dependence, and provide practical formulas for the numerical implementation of our results. We also consider the heavy top mass expansion and show that in the case at hand it converges very slowly.Comment: LaTeX, 29 pages, 6 postscript figures include

    Two-Particle Correlations and B0Bˉ0B^0\bar{B}^0 Mixing

    Full text link
    We study the EPR correlation implied by the entangled wavefunction of the B0Bˉ0B^0\bar{B}^0 pair created by the Υ\Upsilon (4S) resonance. The analysis uses the basis provided by the mass eigenstates B1,B2B_1,B_2 rather than the flavour states B0,Bˉ0B^0, \bar{B}^0. Data on the inclusive dilepton charge ratio are close to the expectation of quantum mechanics, but nearly 8 standard deviations away from that of complete decoherence.Comment: 10 pages, Latex, no figure

    B^0-\bar B^0 Mixing in Gauge-Higgs Unification

    Full text link
    We discuss flavor mixing and resulting Flavor Changing Neutral Current (FCNC) in a five dimensional SU(3)_color \otimes SU(3) \otimes U'(1) gauge-Higgs unification. Flavor mixing is realized by the fact that the bulk and brane localized mass terms are not diagonalized simultaneously. As the concrete FCNC processes, we calculate the rate of B^0_d-\bar B^0_d mixing and B^0_s-\bar B^0_s mixing due to the exchange of non-zero Kaluza-Klein gluons at the tree level. We obtain a lower bound on the compactification scale of order O(TeV) by comparing our prediction on the mass difference of neutral B meson with the recent experimental data.Comment: 18 pages, 6 figures. arXiv admin note: substantial text overlap with arXiv:1103.5980 [hep-ph

    Charge Asymmetry of Same-Sign Dileptons in B0B^0-Bˉ0\bar{B}^0 Mixing

    Full text link
    We report a measurement of the charge asymmetry for same-sign dileptons in B0B^0-Bˉ0\bar{B}^0 mixing, AslA_{\rm sl}. The data were collected with the Belle detector at KEKB. Using a data sample of 78 fb1^{-1} recorded at the Υ(4S)\Upsilon(4S) resonance and 9 fb1^{-1} recorded at an energy 60 MeV below the resonance, we measure Asl=(1.1±7.9(stat)±7.0(sys))×103A_{\rm sl} = (-1.1 \pm 7.9(\text{stat}) \pm 7.0(\text{sys}))\times 10^{-3}.Comment: 21 pages, 9 figures, 3 tables, submitted to Physical Review

    Factorization of the charge correlation function in B0Bˉ0B^0\bar B^0 oscillations

    Full text link
    Extraction of the mass difference Δm\Delta m from B0Bˉ0B^0\bar B^0 oscillations involves tagging of bottom flavour at production and at decay. We show that the asymmetry between the unmixed and mixed events factorizes into two parts, one depending on the production-tag and the other on the decay-tag.Comment: 6 pages, Latex, no figure
    corecore