D.M. Binnie
Imperial College London
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Featured researches published by D.M. Binnie.
Physics Letters B | 1979
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; G. Knop; W. Korbach; P. Leu; B. Löhr; F. Roth; W. Rühmer; R. Wedemeyer; N. Wermes; M. Wollstadt; R. Buhring; R. Fohrmann
Abstract Hadron jets produced in e+e− annihilation between 13 GeV and 31.6 GeV in c.m. at PETRA are analyzed. The transverse momentum of the jets is found to increase strongly with c.m. energy. The broadening of the jets is not uniform in azimuthal angle around the quark direction but tends to yield planar events with large and growing transverse momenta in the plane and smaller transverse momenta normal to the plane. The simple q q collinear jet picture is ruled out. The observation of planar events shows that there are three basic particles in the final state. Indeed, several events with three well-separated jets of hadrons are observed at the highest energies. This occurs naturally when the outgoing quark radiates a hard noncollinear gluon, i.e., e + e − → q q g with the quarks and the gluons fragmenting into hadrons with limited transverse momenta.
Physics Letters B | 1979
R. Brandelik; J. C. Hart; J. Proudfoot; D. Heyland; H.G. Sander; E. Hilger; R. Fohrmann; Jorg Pyrlik; D. H. Saxon; W. Braunschweig; H. Hultschig; A. Ladage; P.J. Dornan; S. L. Lloyd; H.-U. Martyn; D. Revel; G. Mikenberg; H. M. Fischer; Roger J Cashmore; O. Römer; H. Boerner; D. Trines; M. Wollstadt; B. Löhr; Kenneth Watson Bell; G. Poelz; M. Ogg; Roger Barlow; D. A. Garbutt; R. Wedemeyer
Abstract We have observed e + e − hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detector. We find R (13 GeV) = 5.6 ± 0.7 and R (17 GeV) = 4.0 ± 0.7. The additional systematic uncertainty is 20%. Comparing inclusive charged hadron spectra we observe scaling between 5 GeV and 17 GeV for x = p / p beam > 0.2; however the 13 GeV cross section is above the 17 GeV cross section for smaller x . This may be due to copious bb production. The events become increasingly jet like at high energies as evidenced by a shrinking sphericity distribution with increasing energy.
Physics Letters B | 1980
R. Brandelik; A. Pevsner; J. Proudfoot; D. G. Cassel; D. Heyland; H.G. Sander; S. Yarker; E. Hilger; D. R. Quarrie; R. Fohrmann; Jorg Pyrlik; D. H. Saxon; W. Braunschweig; H. Hultschig; A. Ladage; P.J. Dornan; Peter Mattig; H.-U. Martyn; J.K. Sedgbeer; D. Revel; G. Mikenberg; H. M. Fischer; W. Chinowsky; O. Römer; H. Boerner; D. Trines; M. Wollstadt; B. Löhr; Kenneth Watson Bell; G. Poelz
Abstract Hadron production by e + e − annihilation has been studied for c.m. energies W between 13 and 31.6 GeV. As a function of 1n W the charged particle multiplicity grows faster at high energy than at lower energies. This is correlated with a rise in the plateau of the rapidity distribution. The cross section s d σ /d x is found to scale within ±30% for x > 0.2 and 5 ⩽ W ⩽ 31.6 GeV.
Physics Letters B | 1989
W. Braunschweig; R. Gerhards; F. J. Kirschfink; H.-U. Martyn; H. M. Fischer; H. Hartmann; J. Hartmann; E. Hilger; A. Jocksch; R. Wedemeyer; B. Foster; A.J. Martin; E. Bernardi; J. J. Chwastowski; A. Eskreys; K. Genser; H. Hultschig; P. Joos; H. Kowalski; A. Ladage; B. Löhr; D. Lüke; D. Notz; J. M. Pawlak; K. U. Pösnecker; E. Ros; D. Trines; R. Walczak; G. Wolf; H. Kolanoski
Abstract Intermittency effects have been studied directly for the first time in e + e − annihilation, using 37 509 hadronic events at an average CM energy of 〈√ s 〉=35 GeV. The factorial moments F 2 , F 3 and F 4 are given for the rapidity distribution and for the two-dimensional distributions in rapidity and azimuthal angle. The effects of cuts in sphericity and particle momentum are large. Comparison with several fragmentation models are made; some models like the Lund model with O(α s 2 ) matrix element give a qualitative description of the phenomena. The importance of detector effects is demonstrated. The results are discussed in terms of various suggested interpretations of this effect.
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 | 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.
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 A | 1989
W. Braunschweig; R. Gerhards; F. J. Kirschfink; H.-U. Martyn; B. Bock; H. M. Fischer; H. Hartmann; J. Hartmann; E. Hilger; A. Jocksch; R. Wedemeyer; B. Foster; A. J. Martin; A. J. Sephton; F. Barreiro; E. Bernardi; J. J. Chwastowski; A. Eskreys; K. Gather; K. Genser; H. Hultschig; P. Joos; H. Kowalski; A. Ladage; B. Löhr; D. Lüke; P. Mättig; D. Notz; J. M. Pawlak; K. U. Pösnecker
AbstractThe inclusive production of π± andK± mesons and of protons and antiprotons ine+e− annihilations has been measured at 34 GeV and 44 GeV center of mass energy; in addition π± mesons have been measured at 44 GeV c.m. energy. Differential cross sections and particle yields are given. At 34 GeV average multiplicities are: