571 research outputs found

    The NNLO non-singlet QCD analysis of parton distributions based on Bernstein polynomials

    Get PDF
    A non-singlet QCD analysis of the structure function xF3xF_3 up to NNLO is performed based on the Bernstein polynomials approach. We use recently calculated NNLO anomalous dimension coefficients for the moments of the xF3xF_3 structure function in νN\nu N scattering. In the fitting procedure, Bernstein polynomial method is used to construct experimental moments from the xF3xF_3 data of the CCFR collaboration in the region of xx which is inaccessible experimentally. We also consider Bernstein averages to obtain some unknown parameters which exist in the valence quark densities in a wide range of xx and Q2Q^2. The results of valence quark distributions up to NNLO are in good agreement with the available theoretical models. In the analysis we determined the QCD-scale ΛQCD,Nf=4MSˉ=211\Lambda^ {\bar{MS}}_{QCD, N_{f}=4}=211 MeV (LO), 259 MeV (NLO) and 230 MeV (NNLO), corresponding to αs(MZ2)=0.1291\alpha_s(M_Z^2)=0.1291 LO, αs(MZ2)=0.1150\alpha_s(M_Z^2)=0.1150 NLO and αs(MZ2)=0.1142\alpha_s(M_Z^2)=0.1142 NNLO. We compare our results for the QCD scale and the αs(MZ2)\alpha_s(M_Z^2) with those obtained from deep inelastic scattering processes.Comment: 20 pages, 7 figures, published in JHE

    Value of alpha_s from deep-inelastic-scattering data

    Full text link
    We report the value of αs\alpha_{\rm s} obtained from QCD analysis of existing data on deep-inelastic scattering of charged leptons off proton and deuterium and estimate its theoretical uncertainties with particular attention paid to impact of the high-twist contribution to the deep-inelastic-scattering structure functions. Taking into account the major uncertainties the value αsNNLO(MZ)=0.1143±0.0014(exp.)±0.0013(theor.)\alpha^{\rm NNLO}_{\rm s}(M_{\rm Z})=0.1143 \pm 0.0014({\rm exp.})\pm 0.0013({\rm theor.}) is obtained. An extrapolation of the LO--NLO--NNLO results to the higher orders makes it possible to estimate αsN3LO(MZ)0.113\alpha^{\rm N^3LO}_{\rm s}(M_{\rm Z})\sim 0.113.Comment: 9 pages, LATEX, 4 figures (EPS). Talk given at 16th International Baldin Seminar on High-Energy Physics Problems: Relativistic Nuclear Physics and Quantum Chromodynamics (ISHEPP 16), Dubna, Russia, 10-15 Jun 200; v2: typos corrected, layout improved, 2 references adde

    Mining Markov Network Surrogates for Value-Added Optimisation

    Get PDF
    Surrogate fitness functions are a popular technique for speeding up metaheuristics, replacing calls to a costly fitness function with calls to a cheap model. However, surrogates also represent an explicit model of the fitness function, which can be exploited beyond approximating the fitness of solutions. This paper proposes that mining surrogate fitness models can yield useful additional information on the problem to the decision maker, adding value to the optimisation process. An existing fitness model based on Markov networks is presented and applied to the optimisation of glazing on a building facade. Analysis of the model reveals how its parameters point towards the global optima of the problem after only part of the optimisation run, and reveals useful properties like the relative sensitivities of the problem variables

    New Approach to GUTs

    Get PDF
    We introduce a new string-inspired approach to the subject of grand unification which allows the GUT scale to be small, \lesssim 200 TeV, so that it is within the reach of {\em conceivable} laboratory accelerated colliding beam devices. The key ingredient is a novel use of the heterotic string symmetry group physics ideas to render baryon number violating effects small enough to have escaped detection to date. This part of the approach involves new unknown parameters to be tested experimentally. A possible hint at the existence of these new parameters may already exist in the EW precision data comparisons with the SM expectations.Comment: 8 pages; improved text and references, note added; extended text, 1 figure added; extended text for publication in Eur. Phys. Journal

    The 2009 World Average of αs\alpha_s

    Get PDF
    Measurements of αs\alpha_s, the coupling strength of the Strong Interaction between quarks and gluons, are summarised and an updated value of the world average of αs(MZ)\alpha_s (M_Z) is derived. Building up on previous reviews, special emphasis is laid on the most recent determinations of αs\alpha_s. These are obtained from τ\tau-decays, from global fits of electroweak precision data and from measurements of the proton structure function \F_2, which are based on perturbative QCD calculations up to O(αs4)O(\alpha_s^4); from hadronic event shapes and jet production in \epem annihilation, based on O(αs3)O(\alpha_s^3) QCD; from jet production in deep inelastic scattering and from Υ\Upsilon decays, based on O(αs2)O(\alpha_s^2) QCD; and from heavy quarkonia based on unquenched QCD lattice calculations. Applying pragmatic methods to deal with possibly underestimated errors and/or unknown correlations, the world average value of αs(MZ)\alpha_s (M_Z) results in αs(MZ)=0.1184±0.0007\alpha_s (M_Z) = 0.1184 \pm 0.0007. The measured values of αs(Q)\alpha_s (Q), covering energy scales from Q \equiv \mtau = 1.78 GeV to 209 GeV, exactly follow the energy dependence predicted by QCD and therefore significantly test the concept af Asymptotic Freedom.Comment: 14 pages, 7 figure

    Measurement of the partial widths of the Z into up- and down-type quarks

    Full text link
    Using the entire OPAL LEP1 on-peak Z hadronic decay sample, Z -> qbarq gamma decays were selected by tagging hadronic final states with isolated photon candidates in the electromagnetic calorimeter. Combining the measured rates of Z -> qbarq gamma decays with the total rate of hadronic Z decays permits the simultaneous determination of the widths of the Z into up- and down-type quarks. The values obtained, with total errors, were Gamma u = 300 ^{+19}_{-18} MeV and Gamma d = 381 ^{+12}_{-12} MeV. The results are in good agreement with the Standard Model expectation.Comment: 22 pages, 5 figures, Submitted to Phys. Letts.

    Measurement of the Strong Coupling alpha s from Four-Jet Observables in e+e- Annihilation

    Full text link
    Data from e+e- annihilation into hadrons at centre-of-mass energies between 91 GeV and 209 GeV collected with the OPAL detector at LEP, are used to study the four-jet rate as a function of the Durham algorithm resolution parameter ycut. The four-jet rate is compared to next-to-leading order calculations that include the resummation of large logarithms. The strong coupling measured from the four-jet rate is alphas(Mz0)= 0.1182+-0.0003(stat.)+-0.0015(exp.)+-0.0011(had.)+-0.0012(scale)+-0.0013(mass) in agreement with the world average. Next-to-leading order fits to the D-parameter and thrust minor event-shape observables are also performed for the first time. We find consistent results, but with significantly larger theoretical uncertainties.Comment: 25 pages, 15 figures, Submitted to Euro. Phys. J.

    Search for R-Parity Violating Decays of Scalar Fermions at LEP

    Full text link
    A search for pair-produced scalar fermions under the assumption that R-parity is not conserved has been performed using data collected with the OPAL detector at LEP. The data samples analysed correspond to an integrated luminosity of about 610 pb-1 collected at centre-of-mass energies of sqrt(s) 189-209 GeV. An important consequence of R-parity violation is that the lightest supersymmetric particle is expected to be unstable. Searches of R-parity violating decays of charged sleptons, sneutrinos and squarks have been performed under the assumptions that the lightest supersymmetric particle decays promptly and that only one of the R-parity violating couplings is dominant for each of the decay modes considered. Such processes would yield final states consisting of leptons, jets, or both with or without missing energy. No significant single-like excess of events has been observed with respect to the Standard Model expectations. Limits on the production cross- section of scalar fermions in R-parity violating scenarios are obtained. Constraints on the supersymmetric particle masses are also presented in an R-parity violating framework analogous to the Constrained Minimal Supersymmetric Standard Model.Comment: 51 pages, 24 figures, Submitted to Eur. Phys. J.

    Measurement of the Hadronic Photon Structure Function F_2^gamma at LEP2

    Get PDF
    The hadronic structure function of the photon F_2^gamma is measured as a function of Bjorken x and of the factorisation scale Q^2 using data taken by the OPAL detector at LEP. Previous OPAL measurements of the x dependence of F_2^gamma are extended to an average Q^2 of 767 GeV^2. The Q^2 evolution of F_2^gamma is studied for average Q^2 between 11.9 and 1051 GeV^2. As predicted by QCD, the data show positive scaling violations in F_2^gamma. Several parameterisations of F_2^gamma are in agreement with the measurements whereas the quark-parton model prediction fails to describe the data.Comment: 4 pages, 2 figures, to appear in the proceedings of Photon 2001, Ascona, Switzerlan

    Measurement of Rb in e+e- Collisions at 182 - 209 GeV

    Full text link
    Measurements of Rb, the ratio of the bbbar cross-section to the qqbar cross- section in e+e- collisions, are presented. The data were collected by the OPAL experiment at LEP at centre-of-mass energies between 182 GeV and 209 GeV. Lepton, lifetime and event shape information is used to tag events containing b quarks with high efficiency. The data are compatible with the Standard Model expectation. The mean ratio of the eight measurements reported here to the Standard Model prediction is 1.055+-0.031+-0.037, where the first error is statistical and the second systematic.Comment: 21 pages, 5 figures, Submitted to Phys. Letts
    corecore