L. Deck
Max Planck Society
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Featured researches published by L. Deck.
Nuclear Physics | 1983
H. Grässler; D. Lanske; R. Schulte; G. Jones; R.P. Middleton; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; B. Nellen; A. Grant; D.R.O. Morrison; P. Schmid; H. Wachsmuth; J.S. Chima; M.M. Mobayyen; M. Talebzadeh; O. Villalobos-Baillie; M. Aderholz; L. Deck; N. Schmitz; R. Settles; K.L. Wernhard; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells
In an experiment with the hydrogen bubble chamber BEBC at CERN multiplicities of hadrons produced in νp and vp interactions have been investigated. Results are presented on the multiplicities of charged hadrons and neutral pions, forward and backward multiplicities of charged hadrons and correlations between forward and backward multiplicities. Comparisons are made with hadronic reactions and e+e− annihilation. In the framework of the quark-parton model the data imply similar charged multiplicities for the fragments of a u- and a d-quark, and a larger multiplicities for the fragments of a uu- than for a ud-diquark. The correlation data suggest independent fragmentation of the quark and diquark for hadronic masses above ∼ 7 GeV and local charge compensation within an event.
Nuclear Physics | 1986
P. Allen; F. Hamisi; G. Jones; K.W.J. Barnham; E.F. Clayton; P. Schmid; N. Schmitz; E. Hoffmann; W. Wittek; R. Schulte; D. Radojicic; M. Aderholz; D.R.O. Morrison; G. Corrigan; G. Myatt; W. Gebel; H. Wachsmuth; S.J. Towers; B. Saitta; J. Mittendorfer; S. W. O'Neale; L. Deck; D.B. Miller; B. W. Kennedy; M. M. Mobayyen; P.N. Shotton; H. Grässler
Abstract We present results on exclusive single-charged pion and kaon production in neutrino and antineutrino interactions on protons in the energy range from 5 to 120 GeV. The data were obtained from exposures of BEBC to wide band beams at the CERN SPS. For invariant masses of the (pπ) system below 2 GeV, the pions originate predominantly from decays of baryon resonances excited by the weak charged current. Similarly, we observe the production of Λ(1520) decaying into p and K−. For invariant masses above 2 GeV pion production becomes peripheral by interaction of the weak current with a virtual π0. We establish a contribution of longitudinally polarised intermediate vector bosons to this process.
European Physical Journal A | 1985
G. Jones; B. W. Kennedy; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; B. Nellen; A. M. Cooper-Sarkar; A. Grant; D. R. O. Morrison; P. Schmid; H. Wachsmuth; J.S. Chima; M.M. Mobayyen; M. Talebzadeh; O. Villalobos-Baillie; M. Aderholz; L. Deck; N. Schmitz; K.L. Wernhard; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells; S. Towers; P. Shotton
AbstractNeutral kaon to negative pion production ratios fromvp and
European Physical Journal C | 1984
G. Jones; B. W. Kennedy; R. P. Middleton; S. W. O'Neale; A. M. Cooper; A. Grant; J. Mittendorfer; D. R. O. Morrison; A. Parker; P. Schmid; H. Wachsmuth; F. Hamisi; M. M. Mobayyen; O. Villalobos-Baillie; M. Aderholz; L. Deck; N. Schmitz; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; M. Retter
Nuclear Physics | 1986
H. Grässler; D. Lanske; R. Schulte; G. Jones; B. W. Kennedy; R. P. Middleton; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; E. Hoffmann; B. Nellen; H. Saarikko; J. Mittendorfer; D. R. O. Morrison; P. Schmid; H. Wachsmuth; K.W.J. Barnham; E. Clayton; F. Hamisi; D.B. Miller; M.M. Mobayyen; M. Aderholz; L. Deck; N. Schmitz; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta
\bar vp
Nuclear Physics | 1986
H. Grässler; G. Myatt; K.W.J. Barnham; W. Venus; M.L. Faccini-Turluer; B. Wünsch; P. Schmid; N. Schmitz; P. Bostock; Michael Andrew Parker; G.G. Harigel; D. Cundy; U. Idschok; H. Foeth; M. Aderholz; J. Guy; D.R.O. Morrison; W. Droge; W. Wittek; M. M. Mobayyen; J. Krstic; B. Nellen; K. Hultqvist; H. Wachsmuth; A. Vayaki; M. Talebzadeh; D. Radojicic; E. Simopoulou; M. Nikolic; H. Kreutzmann
Physics Letters B | 1986
G. Jones; R. W. L. Jones; B. W. Kennedy; S. W. O'Neale; E. Hoffmann; D. Haidt; J. Mittendorfer; D. R. O. Morrison; P. Schmid; H. Wachsmuth; F. Hamisi; D. B. Miller; M. M. Mobayyen; M. Aderholz; L. Deck; N. Schmitz; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; M.L. Retter; B. Saitta; P.N. Shotton; S.J. Towers; F.W. Bullock; S. Burke; P.J. Fitch
charged current interactions in BEBC are presented and compared with LUND fragmentation model predictions. Good agreement is obtained with a strangeness suppression factor λ=0.203±0.014(stat)±0.010(sys). No evidence is seen for an energy dependence of λ in our kinematic region.
European Physical Journal A | 1985
G. Jones; B. W. Kennedy; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; B. Nellen; Amanda M. Cooper-Sarkar; A. Grant; D. R. O. Morrison; P. Schmid; H. Wachsmuth; K.W.J. Barnham; E. F. Clayton; D.B. Miller; M.M. Mobayyen; O. Villalobos-Baillie; M. Aderholz; L. Deck; N. Schmitz; R. Settles; K.L. Wernhard; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells
Data from a neutrino and antineutrino hydrogen experiment with BEBC are used to investigate transverse properties of the produced charged hadrons. Measurements are presented on average transverse momenta of charged pions as functions of Feynman-x and the hadronic mass, on the transverse momentum flow within an event and on jet-related quantities. The main features of the data are well described by the LUND model. The data favour a version of the model in which soft gluon effects are included and the primordial transverse momentum of the quarks in the proton is small. Effects from 1st order QCD (hard gluon emission) are negligible.
Nuclear Physics | 1986
H. Grässler; D. Lanske; R. Schulte; Goronwy Tudor Jones; B. W. Kennedy; R. P. Middleton; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; E. Hoffmann; B. Nellen; H. Saarikko; J. Mittendorfer; D. R. O. Morrison; Ph. E. Schmid; H. Wachsmuth; K.W.J. Barnham; E. Clayton; F. Hamisi; D.B. Miller; M. M. Mobayyen; M. Aderholz; L. Deck; N. Schmitz; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta
Inclusive ϱ0 production has been studied in antineutrino-proton charged current interactions, using a sample of 3340 events obtained in BEBC filled with hydrogen and exposed to the CERN wideband antineutrino beam. An average multiplicity of 0.11 ± 0.02ϱ0 per event at a mean hadronic mass W of 4.2 GeV is observed. The ϱ0 production characteristics are determined as functions of pT, xF, and z. The ratio ϱ0/“π0” is found to be low at small z values consistent with centrally produced pions coming mainly from resonances. At large z values this ratio approaches 0.45 ± 0.15 which is compatible with a vector/pseudoscalar meson direct production ratio of one. The results are compared with those obtained from neutrino-proton interactions in the same experimental set-up.Inclusive ϱ0 production has been studied in antineutrino-proton charged current interactions, using a sample of 3340 events obtained in BEBC filled with hydrogen and exposed to the CERN wideband antineutrino beam. An average multiplicity of 0.11 ± 0.02ϱ0 per event at a mean hadronic mass W of 4.2 GeV is observed. The ϱ0 production characteristics are determined as functions of pT, xF, and z. The ratio ϱ0/“π0” is found to be low at small z values consistent with centrally produced pions coming mainly from resonances. At large z values this ratio approaches 0.45 ± 0.15 which is compatible with a vector/pseudoscalar meson direct production ratio of one. The results are compared with those obtained from neutrino-proton interactions in the same experimental set-up.
Archive | 1985
Gary Tyson Jones; B. W. Kennedy; S. W. O'Neale; K. Böckmann; W. Gebel; C. Geich-Gimbel; B. Nellen; A. M. Cooper-Sarkar; A. Grant; R. Klein; D.R.O. Morrison; P. Schmid; H. Wachsmuth; Keith W J Barnham; E. Clayton; D.B. Miller; M. M. Mobayyen; O Villalobos Baillie; M. Aderholz; L. Deck; N. Schmitz; Ronald Settles; K.L. Wernhard; Werner Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells
Abstract The prompt electron neutrino and muon neutrino fluxes from proton copper interactions at 400 GeV/ c proton momentum have been measured. The asymmetry between the prompt electron (anti) neutrino and the prompt muon (anti) neutrino event rates above 20 GeV is A e μ = (N e − N μ (N c + N μ ) = 0.07 ± 0.08 corresponding to an N e / N μ ratio of 1.14 −0.16 −0.19 . The cross section weighted charge asymmetry for electrons and muons combined is A ν ν = 0.15 ± 0.08 . The number of D decays into ν e and ν μ is (4.1 ± 0.9) × 10 −4 per incident proton. No evidence for ν τ interactions was found.