4,421 research outputs found

    K_l3 form factor with two-flavors of dynamical domain-wall quarks

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    We report on our calculation of K \to \pi vector form factor by numerical simulations of two-flavor QCD on a 16^3x32x12 lattice at a \simeq 0.12 fm using domain-wall quarks and DBW2 glue. Our preliminary result at a single sea quark mass correponding to m_PS/m_V \simeq 0.53 shows a good agreement with previous estimate in quenched QCD and that from a phenomenological model.Comment: 6 pages, 5 figures, poster presented at Lattice2005 (Weak matrix elements); v2: a reference adde

    SU(3) Flavor Breaking in Hadronic Matrix Elements for B−BˉB - \bar B Oscillations

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    We present an analysis, using quenched configurations at 6/g2=6/g^2=5.7, 5.85, 6.0, and 6.3 of the matrix element \MP\equiv\langle \bar P_{hl}|\bar h \gamma_\mu (1-\gamma_5)l \bar h \gamma_\mu(1-\gamma_5)l|P_{hl}\rangle for heavy-light pseudoscalar mesons. The results are extrapolated to the physical BB meson states, \Bd and \Bs. We directly compute the ratio \MS/\MB, and obtain the preliminary result \MS/\MB=1.54(13)(32). A precise value of this SU(3) breaking ratio is important for determining VtdV_{td} once the mixing parameter xsx_s for \Bs-\bar\Bs is measured experimentally. We also determine values for the corresponding B parameters, Bbs(2GeV)=Bbd(2GeV)=1.02(13)B_{bs}(2 \rm{GeV})=B_{bd}(2 \rm{GeV})=1.02(13), which we cannot distinguish in the present analysis.Comment: Poster presented at LATTICE96(heavy quarks). LaTeX, uses espcrc2.sty and epsf, 4 pages, 4 postscript figures include

    Semi-inclusive hadronic B decays as null tests of the Standard Model

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    We propose a new set of observables that can be used as experimental null tests of the Standard Model in charged and neutral B decays. The CP asymmetries in hadronic decays of charged B mesons into inclusive final states containing at least one of the following mesons: K_{S,L}, eta', c\bar c bound states or neutral K^* or D mesons, for all of which a U-spin rotation is equivalent to a CP conjugation, are CKM suppressed and furthermore vanish in the exact U-spin limit. We show how this reduces the theoretical error by using Soft Collinear Effective Theory to calculate the CP asymmetries for K_{S,L} X_{s+d}, K^* X_{s+d} and eta' X_{s+d} final states in the endpoint region. For these CP asymmetries only the flavor and not the charge of the decaying B meson needs to be tagged up to corrections of NLO in 1/m_b, making the measurements more accessible experimentally.Comment: 8 pages, significantly expanded after the observation that both neutral and charged B decays can be used, calculation for decays involving eta' adde

    Calculation of the neutron electric dipole moment with two dynamical flavors of domain wall fermions

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    We present a study of the neutron electric dipole moment (d⃗N\vec d_N) within the framework of lattice QCD with two flavors of dynamical lig ht quarks. The dipole moment is sensitive to the topological structure of the gaug e fields, and accuracy can only be achieved by using dynamical, or sea quark, calc ulations. However, the topological charge evolves slowly in these calculations, le ading to a relatively large uncertainty in d⃗N\vec d_N. It is shown, using quenched configurations, that a better sampling of the charge d istribution reduces this problem, but because the CP even part of the fermion determinant is absent, both the topological charge dis tribution and d⃗N\vec d_N are pathological in the chiral limit. We discuss the statistical and systematic uncertainties arising from the topological charge distr ibution and unphysical size of the quark mass in our calculations and prospects fo r eliminating them. Our calculations employ the RBC collaboration two flavor domain wall fermion and DBW2 gauge action lattices with inverse lattice spacing a−1≈a^{-1}\approx 1.7 GeV, physical volume V≈(2V\approx (2 fm)3^3, and light quark mass roughly equal to the strange quark mass (msea=0.03m_{sea}=0.03 and 0.04). We determine a value of the electric dipole moment that is zero withi n (statistical) errors, ∣d⃗N∣=−0.04(20)|\vec d_N| = -0.04(20) e-θ\theta-fm at the smaller sea quark mass. Satisfactory results for the magnetic and electric form factors of the proton and neutron are also obtained and presented.Comment: 46 pages. Changed one author addres
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