R. C. E. Devenish
University of Oxford
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Featured researches published by R. C. E. Devenish.
Physics Letters B | 1980
R. Brandelik; W. Braunschweig; K. Gather; Kadansky; K. Lübelsmeyer; P. Mättig; H.-U. Martyn; G. Peise; J. Rimkus; H.G. Sander; D. Schmitz; A. Schultz von Dratzig; D. Trines; W. Wallraff; H. Boerner; H. M. Fischer; H. Hartmann; E. Hilger; W. Hillen; L. Koepke; G. Knop; P. Leu; B. Löhr; R. Wedemeyer; N. Wermes; M. Wollstadt; H. Burkhardt; D. G. Cassel; D. Heyland; H. Hultschig
We have analyzed 1113 events of the reaction e+e− → hadrons at CM energies of 12 and 30 GeV in order to make a detailed comparison with QCD. Perturbative effects can be well separated from effects depending on the quark and gluon fragmentation parameters to yield a reliable measurement of the coupling constant αS. At 30 GeV, the result is αS = 0.17 ± 0.02 (statistical) ± 0.03 (systematic). QCD model predictions, using the fragmentation parameters determined along with αS, agree with both gross properties of the final states and with detailed features of the three-jet states.
Physics Letters B | 1980
R. Brandelik; W. Braunschweig; K. Gather; V. Kadansky; F. J. Kirschfink; K. Lübelsmeyer; H.-U. Martyn; G. Peise; J. Rimkus; H. G. Sander; D. Schmitz; A. Schultz von Dratzig; D. Trines; W. Wallraff; H. Boerner; H. M. Fischer; H. Hartmann; E. Hilger; W. Hillen; G. Knop; L. Koepke; H. Kolanoski; P. Leu; B. Löhr; R. Wedemeyer; N. Wermes; M. Wollstadt; H. Burkhardt; D. G. Cassel; D. Heyland
High-energy e+e--annihilation events obtained in the TASSO detector at PETRA have been used to determine the spin of the gluon in the reaction e+e- → qqg. We analysed angular correlations between the three jet axes. While vector gluons are consistent with the data (55% confidence limit), scalar gluons are disfavoured by 3.8 standard deviations, corresponding to a confidence level of about 10-4. Our conclusion is free of possible biases due to uncertainties in the fragmentation process or in determining the qqg kinematics from the observed hadrons.
Physics Letters B | 1983
M. Althoff; W. Braunschweig; K. Gather; F. J. Kirschfink; K. Lübelsmeyer; H.-U. Martyn; G. Peise; J. Rimkus; H. G. Sander; D. Schmitz; H. Siebke; D. Trines; W. Wallraff; H. M. Fischer; H. Hartmann; E. Hilger; W. Hillen; G. Knop; L. Köpke; H. Kolanoski; H. Kück; R. Wedemeyer; N. Wermes; M. Wollstadt; H. Burkhardt; H. Hultschig; P. Joos; W. Koch; U. Kötz; H. Kowalski
Abstract D∗± production via e+e−→D∗±X has been measured at an average CM energy of 34.4 GeV. The D∗± energy spectrum is hard, with a maximum near χ = 0.6. The size of the D∗ cross section, R D ∗ = σ( e + e − → D ∗ X ) σ μμ = 2.50 ± 0.64 ± 0.88 (assuming R D ∗0 = R D ∗+ ) indicates that a large fraction of charm quark production yields D∗ mesons. The D∗± angular distribution exhibits a forward—backward asymmetry, A = −0.28 ± 0.13. This is consistent with that expected in the standard theory for weak neutral currents and leads to |gAc| = 0.89 ± 0.44 for the axial vector coupling of the charm quark.
Physics Letters B | 1982
R. Brandelik; I. Brock; J. Freeman; H. G. Sander; R. Beuselinck; H. Hultschig; H. Burkhardt; P. Mättig; H.-U. Martyn; E. Wicklund; D. Revel; R.A. Stern; A. Shapira; D. Trines; R. Wedemeyer; L. Köpke; D.A. Garbutt; C. Youngman; J.K. Sedgbeer; T. R. Wyatt; H. Kolanoski; D. Lüke; R. Fohrmann; R. Carnegie; F. J. Kirschfink; P. Söding; K. Lübelsmeyer; D. Pandoulas; H. L. Lynch; W.G. Jones
Abstract The ration R = σ (e + e − → hadrons) σ μμ was measured between 12.0 and 36.7 GeV c.m. energy W with a precision of typically ± 5.2%. R is found to be constant with an average R = 4.01 ± 0.03 (stat) ± (syst.) for W ⩾ 14 GeV. Quarks are found to be point-like, the mass parameter describing a possible quark form-factor being larger than 186 GeV. Fits including QCD corrections and a weak neutral-current contribution are presented.
Physics Letters B | 1980
R. Brandelik; W. Braunschweig; K. Gather; V. Kadansky; K. Lübelsmeyer; P. Mättig; H.-U. Martyn; G. Peise; J. Rimkus; H. G. Sander; D. Schmitz; A. Schultz von Dratzig; D. Trines; W. Wallraff; H. Boerner; H. M. Fischer; H. Hartmann; E. Hilger; W. Hillen; L. Koepke; H. Kolanoski; G. Knop; P. Leu; B. Löhr; R. Wedemeyer; N. Wermes; M. Wollstadt; H. Burkhardt; D. G. Cassel; D. Heyland
Abstract Production of pions, kaons, protons and antiprotons has been studied in e + e − annihilations at 12 and 30 GeV centre of mass energy using time of flight techniques. The fractional yield of charged kaons and baryons appears to rise with outgoing particle momentum. At our highest energy at least 40% of e + e − annihilations into hadrons are estimated to contain baryons.
Physics Letters B | 1982
R. Brandelik; E. Lohrmann; I. Brock; H. G. Sander; R. Beuselinck; H. Hultschig; H. Burkhardt; P. Mättig; H.-U. Martyn; E. Wicklund; D. Revel; A. Shapira; D. Trines; R. Wedemeyer; L. Köpke; D.A. Garbutt; C. Youngman; J.K. Sedgbeer; T. R. Wyatt; H. Kolanoski; D. Lüke; R. Fohrmann; R. Carnegie; F. J. Kirschfink; P. Söding; K. Lübelsmeyer; D. Pandoulas; H. L. Lynch; W.G. Jones; W. Schütte
Abstract A high statistics experiment was performed on Bhabha scattering at energies between 14 and 34 GeV. Good agreement with QED was observed. The combined data on Bhabha scattering and μ pair production were found to agree with the standard theory of electroweak interaction giving sin2 θ = 0.27−0.07+0.06. Assuming for the Z0 mass a value of 90 GeV the leptonic weak coupling constants were determined to gV2 = −0.04 ± 0.06 and gA2 = 0.35 ± 0.09. A search for scalar leptons sets lower limits on the mass of scalar electrons ofMse > 16.6 GeV and of scalar muons of Msμ > 16.4 GeV.
European Physical Journal C | 1985
M. Althoff; W. Braunschweig; F. J. Kirschfink; H.-U. Martyn; R. Rosskamp; H. Siebke; W. Wallraff; J. Eisenmann; H. M. Fischer; H. Hartmann; A. Jocksch; G. Knop; H. Kolanoski; H. Kück; V. Mertens; R. Wedemeyer; B. Foster; Andrew T. A. Wood; E. Bernardi; Y. Eisenberg; A. Eskreys; R. Fohrmann; K. Gather; H. Hultschig; P. Joos; B. Klima; U. Kötz; H. Kowalski; A. Lagage; B. Löhr
We have studied the correlations between charged particles produced ine+e− annihilations into hadrons at c.m. energies between 29 and 37 GeV. We have analysed the correlations between the charged multiplicities of the jets and the two particle rapidity and charge correlations. No evidence for correlations between the multiplicities of the two jets is found. Two particle short range rapidity and charge correlations are observed, indicating that particles cluster in rapidity and that their charges compensate locally. An extensive study of these correlation effects by QCD Monte Carlo calculations was performed. Evidence for charge correlations due to Bose-Einstein statistics is also observed.
European Physical Journal C | 1986
M. Althoff; W. Braunschweig; F. J. Kirschfink; H.-U. Martyn; P. Rosskamp; W. Wallraff; J. Eisenmann; H. M. Fischer; H. Hartmann; A. Jocksch; G. Knop; H. Kolanoski; H. Kück; V. Mertens; R. Wedemeyer; B. Foster; Andrew T. A. Wood; E. Bernardi; A. Eskreys; R. Fohrmann; K. Gather; H. Hultschig; P. Joos; U. Karshon; B. Klima; U. Kötz; H. Kowalski; A. Ladage; B. Löhr; D. Lüke
Bose-Einstein correlations between pairs of charged particles produced ine+e− annihilation into hadronic final states have been studied as a function ofQ2, the relative momentum squared of the two particles in their centre of mass, and as functions of various pairs of kinematic variables. The observed Bose-Einstein enhancement reveals correlation between the position and time of particle emission, and the space-time structure of the source is shown to differ from that of a pion fireball. While most features of the data are well accounted for in terms of the space-time structure of a simple string model, the correlations are better described by the simple function 1+αe−βQ2. The implications of this result are discussed. The principal features of three particle correlations are explained in terms of the structure of the source inferred from the observed two particle correlations.
European Physical Journal C | 1986
M. Althoff; W. Braunschweig; R. Gerhards; F. J. Kirschfink; H.-U. Martyn; P. Rosskamp; W. Wallraff; B. Bock; J. Eisenmann; H. M. Fischer; H. Hartmann; W. Hillen; A. Jocksch; H. Kolanoski; H. Kück; V. Mertens; R. Wedemeyer; B. Foster; E. Bernardi; Y. Eisenberg; A. Eskreys; K. Gather; H. Hultschig; P. Joos; B. Klima; H. Kowalski; A. Ladage; B. Löhr; D. Lueke; P. Mättig
AbstractWe have measured the processe+e−→e+e−+hadrons, where one of the scattered electrons was detected at large angles, withQ2 ranging from 7 to 70 (VeV/c)2. The photon structure functionF2γ(x, Q2) was determined at an averageQ2 of 23 (GeV/c)2. The measurements were compared to theoretical predictions of the Quark Parton Model and Quantum Chromodynamics. In both models a hadronic part was added. Within the errors the data are in agreement with the QPM using quark masses of 300 MeV/c2 for the light quarks. The data also agree with a QCD calculation including higher order corrections. A fit yielded a
Physics Letters B | 1982
R. Brandelik; W. Braunschweig; K. Gather; F. J. Kirschfink; K. Lübelsmeyer; H.-U. Martyn; G. Peise; J. Rimkus; H. G. Sander; D. Schmitz; H. Siebke; D. Trines; W. Wallraff; H. Boerner; H. M. Fischer; H. Hartmann; E. Hilger; W. Hillen; G. Knop; L. Köpke; H. Kolanoski; R. Wedemeyer; N. Wermes; M. Wollstadt; H. Burkhardt; S. Cooper; J. Franzke; D. Heyland; H. Hultschig; P. Joos