9,449 research outputs found

    Sea quark effects in B Spectroscopy and Decay Constants

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    We present comprehensive results for the spectrum and decay constants of hadrons containing a single b quark. The heavy quark is simulated using an O(1/M)O(1/M) NRQCD action and the light quark using the O(a)O(a) tadpole-improved clover action on gauge configurations containing two degenerate flavours of sea quarks at βnf=2=5.6\beta^{n_f=2}=5.6 provided by the HEMCGC collaboration. We present detailed results for the lower lying SS and PP wave BB meson states and the Λb\Lambda_b baryon. We find broad agreement with experiment. In addition, we present results for the pseudoscalar and, for the first time, the vector decay constants fully consistent to O(α/M):fB=186(5)(stat)(19)(pert)(9)(disc)(13)(NRQCD)(+50)(a−1)MeV,fB∗=181(6)(stat)(18)(pert)(9)(disc)(13)(NRQCD)(+55)(a−1)MeVO(\alpha/M): f_B = 186(5)(stat)(19)(pert)(9)(disc)(13)(NRQCD)(+50)(a^{-1})MeV, f_B^* = 181(6) (stat)(18)(pert)(9)(disc)(13)(NRQCD)(+55)(a^{-1})MeV and fBs/fB=1.14(2)(stat)(−2)(κs)f_{B_s}/f_B = 1.14(2)(stat)(-2)(\kappa_s). We present an investigation of sea quark effects in the BB spectrum and decay constants. We compare our results with those from similar quenched simulations at βnf=0=6.0\beta^{n_f=0}=6.0. For the spectrum, the quenched results reproduce the experimental spectrum well and there is no significant difference between the quenched and nf=2n_f=2 results. For the decay constants, our results suggest that sea quark effects may be large. We find that fBf_B increases by approximately 25% between nf=0n_f=0 and nf=2n_f=2.Comment: 49 pages, 16 figures, revtex, the discussion of systematic errors and the comparison of the pseudoscalar decay constant at nf=0 and nf=2 has been expande

    Potential Models for Radiative Rare B Decays

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    We compute the branching ratios for the radiative rare decays of B into K-Meson states and compare them to the experimentally determined branching ratio for inclusive decay b -> s gamma using non relativistic quark model, and form factor definitions consistent with HQET covariant trace formalism. Such calculations necessarily involve a potential model. In order to test the sensitivity of calculations to potential models we have used three different potentials, namely linear potential, screening confining potential and heavy quark potential as it stands in QCD.We find the branching ratios relative to the inclusive b ->s gamma decay to be (16.07\pm 5.2)% for B -> K^* (892)gamma and (7.25\pm 3.2)% for B -> K_2^* (1430)gamma for linear potential. In the case of the screening confining potential these values are (19.75\pm 5.3)% and (4.74\pm 1.2)% while those for the heavy quark potential are (11.18\pm 4.6)% and (5.09\pm 2.7)% respectively. All these values are consistent with the corresponding present CLEO experimental values: (16.25\pm 1.21)% and (5.93\pm 0.46)%.Comment: RevTeX, 6 pages, 1 eps figur

    Precision Charmonium Spectroscopy From Lattice QCD

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    We present results for Charmonium spectroscopy using Non-Relativistic QCD (NRQCD). For the NRQCD action the leading order spin-dependent and next to leading order spin-independent interactions have been included with tadpole-improved coefficients. We use multi-exponential fits to multiple correlation functions to extract ground and excited SS states. Splittings between the lowest SS, PP and DD states are given and we have accurate values for the SS state hyperfine splitting and the χc\chi_c fine structure. Agreement with experiment is good - the remaining systematic errors are discussed.Comment: 23 pages uuencoded latex file. Contains figures in late

    B meson leptonic decay constant with quenched lattice NRQCD

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    We present a lattice NRQCD study of the B meson decay constant in the quenched approximation with emphasis given to the scaling behavior. The NRQCD action and the heavy-light axial current we use include all terms of order 1/M and the perturbative O(αsa)O(\alpha_s a) and O(αs/M)O(\alpha_s/M) corrections. Using simulations at three value of couplings β\beta=5.7, 5.9 and 6.1 on lattices of size 123×32,163×4812^3\times 32, 16^3\times 48 and 243×6424^3\times 64, we find no significant aa dependence in fBf_B if the O(αsa)O(\alpha_s a) correction is included in the axial current. We obtain fB=167(7)(15)f_B = 167(7)(15) MeV, fBs=191(4)(17)(−0+4)f_{B_s}= 191(4)(17)(^{+4}_{-0}) MeV and fBs/fB=1.15(3)(1)(−0+3)f_{B_s}/f_B =1.15(3)(1)(^{+3}_{-0}), with the first error being statistical, the second systematic, and the third due to uncertainty of strange quark mass, while quenching errors being not included.Comment: 31 pages, 24 eps figure

    f_B with lattice NRQCD including O(1/m_Q^2) corrections

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    We calculate the heavy-light meson decay constant using lattice NRQCD action for the heavy quark and Wilson quark action for the light quark over a wide range in the heavy quark mass. Simulations are carried out on a 16^3 x 32 lattice with 120 quenched gauge configurations generated with the plaquette action at beta=5.8. For the heavy quark part of the calculation, two sets of lattice NRQCD action and current operator are employed. The first set includes terms up to O(1/m_Q) both in the action and the current operator, and the second set up to O(1/m_Q^2), where m_Q is the bare mass of the heavy quark. Tree-level values with tadpole improvement are employed for the coefficients in the expansion. We compare the results obtained from the two sets in detail and find that the truncation error of higher order relativistic corrections for the decay constant are adequately small around the mass of the b quark. We also calculate the 1S hyperfine splitting of B meson, M_{B_s} - M_B and f_{B_s}/f_B with both sets and find that the 1/m_Q^2 corrections are negligible. Remaining systematic errors and the limitation of NRQCD theory are discussed.Comment: 27 pages, 15 figures, RevTex, psfig.sty require

    Influenza and respiratory syncytial virus infections in British Hajj pilgrims

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    Viral respiratory infections including influenza and respiratory syncytial virus (RSV) have been reported during the Hajj among international pilgrims. To help establish the burden of these infections at the Hajj, we set up a study to confirm these diagnoses in symptomatic British pilgrims who attended the 2005 Hajj. UK pilgrims with symptoms of upper respiratory tract infection (URTI) were invited to participate; after taking medical history, nasal swabs were collected for point-of-care testing (PoCT) of influenza and for subsequent PCR analysis for influenza and RSV. Of the 205 patients recruited, 37 (18%) were positive for either influenza or RSV. Influenza A (H3) accounted for 54% (20/37) of the virus-positive samples, followed by RSV 24% (9/37), influenza B 19% (7/37), and influenza A (H1) 3% (1/37). Of the influenza-positive cases, 29% (8/28) had recently had a flu immunisation. Influenza was more common in those who gave a history of contact with a pilgrim with a respiratory illness than those who did not (17 versus 9%). The overall rate of RSV was 4% (9/202). This study confirms that influenza and RSV cause acute respiratory infections in British Hajj pilgrims. Continuing surveillance and a programme of interventions to contain the spread of infection are needed at the Hajj, particularly when the world is preparing for an influenza pandemic

    Quantum statistical properties of some new classes of intelligent states associated with special quantum systems

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    Based on the {\it nonlinear coherent states} method, a general and simple algebraic formalism for the construction of \textit{`ff-deformed intelligent states'} has been introduced. The structure has the potentiality to apply to systems with a known discrete spectrum as well as the generalized coherent states with known nonlinearity function f(n)f (n). As some physical appearance of the proposed formalism, a few new classes of intelligent states associated with \textit{`center of-mass motion of a trapped ion'}, \textit{`harmonious states'} and \textit{`hydrogen-like spectrum'} have been realized. Finally, the nonclassicality of the obtained states has been investigated. To achieve this purpose the quantum statistical properties using the Mandel parameter and the squeezing of the quadratures of the radiation field corresponding to the introduced states have been established numerically.Comment: 13page

    The Semileptonic Decays B→πlνB\to\pi l\nu and D→πlνD\to\pi l\nu from Lattice QCD

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    We present a lattice QCD calculation of the form factors and differential decay rates for semileptonic decays of the heavy-light mesons BB and DD to the final state πlν\pi l\nu. The results are obtained with three methodological improvements over previous lattice calculations: a matching procedure that reduces heavy-quark lattice artifacts, the first study of lattice-spacing dependence, and the introduction of kinematic cuts to reduce model dependence. We show that the main systematics are controllable (within the quenched approximation) and outline how the calculations could be improved to aid current experiments in the determination of~∣Vub∣|V_{ub}| and~∣Vcd∣|V_{cd}|.Comment: 35 pp, 12 fig

    Heavy-Light Mesons with Quenched Lattice NRQCD: Results on Decay Constants

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    We present a quenched lattice calculation of heavy-light meson decay constants, using non-relativistic (NRQCD) heavy quarks in the mass region of the bb quark and heavier, and clover-improved light quarks. The NRQCD Hamiltonian and the heavy-light current include the corrections at first order in the expansion in the inverse heavy quark mass. We study the dependence of the decay constants on the heavy meson mass MM, for light quarks with the tree level (cSWc_{SW} = 1), as well as the tadpole improved clover coefficient. We compare decay constants from NRQCD with results from clover (cSW=1c_{SW}=1) heavy quarks. Having calculated the current renormalisation constant ZAZ_A in one-loop perturbation theory, we demonstrate how the heavy mass dependence of the pseudoscalar decay constants changes after renormalisation. For the first time, we quote a result for fBf_B from NRQCD including the full one-loop matching factors at O(α/M)O(\alpha/M).Comment: 45 pages, latex, 24 postscript figure
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