Showing papers by "L. Köpke published in 1992"

The detector simulation program for the OPAL experiment at LEP

Abstract: The Monte Carlo program for the OPAL experiment at the LEP ee collider is described. This program is based on the GEANT simulation package. The general organization of the program is outlined, and a description is given of the techniques used for simulating the various subdetectors of OPAL. The performance of the program is illustrated by comparisons with recent data recorded by OPAL at LEP. (Submitted to Nucl. Instr. and Meth.) School of Physics and Space Research, University of Birmingham, Birmingham, B15 2TT, UK Dipartimento di Fisica dell' Universit a di Bologna and INFN, Bologna, 40126, Italy CNAF-INFN, Bologna, Italy Physikalisches Institut, Universitat Bonn, D-5300 Bonn 1, FRG Department of Physics, University of California, Riverside, CA 92521 USA Cavendish Laboratory, Cambridge, CB3 0HE, UK Carleton University, Dept of Physics, Colonel By Drive, Ottawa, Ontario K1S 5B6, Canada Centre for Research in Particle Physics, Carleton University, Ottawa, Ontario K1S 5B6, Canada CERN, European Organisation for Particle Physics, 1211 Geneva 23, Switzerland Enrico Fermi Institute and Department of Physics, University of Chicago, Chicago Illinois 60637, USA Fakult at f ur Physik, Albert Ludwigs Universitat, D-7800 Freiburg, FRG Universitat Hamburg/DESY, II Inst. f ur Experimental Physik, 2000 Hamburg 52, FRG Physikalisches Institut, Universitat Heidelberg, Heidelberg, FRG Queen Mary and West eld College, University of London, London, E1 4NS, UK University College London, London, WC1E 6BT, UK Department of Physics, Schuster Laboratory, The University, Manchester, M13 9PL, UK Department of Physics and Astronomy, University of Maryland, College Park, Maryland 20742, USA Laboratoire de Physique Nucl eaire, Universit e de Montr eal, Montr eal, Quebec, H3C 3J7, Canada Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire, OX11 0QX, UK DPhPE, CEN Saclay, F-91191 Gif-sur-Yvette, France International Centre for Elementary Particle Physics, University of Tokyo, Tokyo 113, Japan Brunel University, Uxbridge, Middlesex, UB8 3PH UK Nuclear Physics Department, Weizmann Institute of Science, Rehovot, 76100, Israel Present address: EPFL, Lausanne, Switzerland Present address: Applied Silicon Inc, Ottawa, Canada Present address: Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire, OX11 0QX, UK On leave from Birmingham University, Birmingham B15 2TT, UK Present address: Culham Laboratory, Culham, Oxfordshire, UK Present address: Meiji Gakuin University, Yokohama 244, Japan

A Study of charged particle multiplicities in hadronic decays of the Z0

Abstract: We present an analysis of multiplicity distributions of charged particles produced inZ 0 hadronic decays. The results are based on the analysis of 82941 events collected within 100 MeV of theZ 0 peak energy with the OPAL detector at LEP. The charged particle multiplicity distribution, corrected for initial-state radiation and for detector acceptance and resolution, was found to have a mean 〈n ch〉=21.40±0.02(stat.)±0.43(syst.) and a dispersionD=6.49±0.02(stat.)±0.20(syst.). The shape is well described by the Lognormal and Gamma distributions. A negative binomial parameterisation was found to describe the shape of the multiplicity distribution less well. A comparison with results obtained at lower energies confirms the validity of KNO(-G) scaling up to LEP energies. A separate analysis of events with low sphericity, typically associated with two-jet final states, shows the presence of features expected for models based on a stochastic production mechanism for particles. In all cases, the features observed in the data are well described by the Lund parton shower model JETSET.

A global determination of {Mathematical expression} at LEP

Abstract: The value of the strong coupling constant, $$\alpha _s (M_{Z^0 } )$$ , is determined from a study of 15 different observables in hadronicZ 0 and τ decays. The study includes global event shape variables, jet production rates, energy correlations, theZ 0 line shape and decay asymmetries and the hadronic branching fraction of τ-leptons. Differences between the αs values from the different observables can be consistently attributed to unknown higher order contributions to the calculations. These uncertaities may be parametrized by variations of the renormalization scale and of the parton virtuality to which the data are corrected, separately for each observable, resulting in a consistent description of the event shapes, jet rates and energy correlations with the value $$\alpha _s (M_{Z^0 } ) = 0.122_{ - 0.005}^{ + 0.006} $$ in . The error is dominated by the theoretical uncertainties. Application of recent calculations which include the resummation of leading and next-to-leading logarithms to all orders for some observables confirm this result with a reduced sensitivity to renormalization scale variations. TheZ 0 line shapes and τ-lepton branching ratios yield $$\alpha _s (M_{Z^0 } ) = 0.148 \pm 0.021$$ and $$\alpha _s (M_{Z^0 } ) = 0.123_{ - 0.007}^{ + 0.006} $$ , respectively, in . These measurements and their uncertainties are entirely independent of each other and from event shape and jet observables; the good agreement of the resulting αs values thus constitutes an important consistency check of the reliability of perturbative QCD.

Inclusive neutral vector meson production in hadronic Z0 decays

Abstract: Results are reported of a study of neutral vector meson production in multihadronicZ0 decays in the OPAL experiment at LEP. Pions and kaons have been identified by specific ionisation energy loss andK±π∓ andK+K− mass spectra have been fitted, in bins of the scaled momentum variablexp, to combinations of resonance signals and non-resonant backgrounds. Rates are given forK*(892)° and o(1020), and production cross sections are compared to the predictions of Monte Carlo models. Overall multiplicities have been determined as 0.76±0.07±0.06K*(892)° and 0.086±0.015±0.010 o(1020) per hadronicZ0 decay (the quoted errors are respectively statistical and systematic). Momentum dependent distortions of the ππ mass spectra, possibly associated indirectly with Bose-Einstein effects, have prevented reliable measurement of the ρ(770)° cross section in this study.

A measurement of electron production in hadronic Z0 decays and a determination of {Mathematical expression}

Abstract: The production rate of electrons with momentump>4 GeV/c and large momentum transverse to the jet containing the electron has been measured in 136000 hadronic decays of theZ 0 recorded with the OPAL detector at LEP in 1990. The dominant source of these electrons is the semileptonic decay of hadrons containingb quarks. If we assume that the semileptonic branching fraction ofb hadrons produced on theZ 0 resonance is the same as the branching fraction measured at the ϒ(4S) resonance, we determine $$\Gamma _{b\bar b} = 394 \pm 13 \pm 32$$ MeV, where the first error is statistical and the second error is systematic. The sensitivity of the result to this assumption is discussed. We have reduced the dependence of our result on the model ofb hadron semileptonic decay by taking into account the correlation between the model dependence of the branching fractions measured at the ϒ(4S) and of our kinematic acceptance for electrons.

Properties of multihadronic events with a final state photon at {Mathematical expression}

Abstract: The properties of final state photons in multihadronic decays of theZ0 and those of the recoiling hadronic system are discussed and compared with theoretical expectations. The yield of two and three jet events with final state photons is found to be in good agreement with the expectation from a matrix element calculation ofO(ααs. Uncertainties in the interpretation of the theoretical calculation do not yet permit a final assessment of events with just one reconstructed jet. Comparing the rates of two jet events with a photon to those of three jet events in the inclusive multihadronic sample, the strong coupling constant in second order is determined asαs\((M_{Z^0 } )\)=0.122±0.010, taking into account only the statistical and experimental systematic errors. It is found that an abelian model of the strong interaction does not describe the data. The comparison of the total yield and the jet rates with QCD shower programs shows better agreement with the ARIADNE model than with the JETSET model. Both programs are found to describe well the photon properties and the properties of the residual hadronic event.