G. Myatt
Max Planck Society
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Featured researches published by G. Myatt.
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 | 1981
P. Allen; J. Blietschau; H. Grässler; D. Lanske; R. Schulte; H.H. Seyfert; K. Böckmann; C. Geich-Gimbel; T. P. Kokott; B. Nellen; R. Pech; H. Saarikko; P. Bosetti; V.T. Cocconi; B. Conforto; A. Grant; P.O. Hulth; G. Kellner; D. R. O. Morrison; R. Orava; L. Pape; P. Schmid; W.G. Scott; H. Wachsmuth; M. Aderholz; N. Schmitz; R. Settles; K.L. Wernhard; W. Wittek; R. Batley
Abstract Multiplicity distributions of charged hadrons produced in νp interactions are studied using a sample of 7850 charged current interactions in BEBC. Multiplicity moments are studied as functions of the invariant mass of the hadronic system, W , and a comparison is made with other lepton- and hadron-induced reactions. The mean charged multiplicity 〈 n ch 〉 is found to increase linearly with ln W 2 . The other multiplicity moments indicate a close similarity between the neutrino scattering and the class of annihilation processes. A study of the multiplicity distributions in the forward and backward directions in the hadronic c.m.s. gives results in qualitative agreement with the quark parton model.
Nuclear Physics | 1983
P. Allen; H. Grässler; D. Lanske; R. Schulte; K. Böckmann; C. Geich-Gimbel; B. Nellen; H. Saarikko; A. Grant; D. R. O. Morrison; P. Schmid; H. Wachsmuth; M. Aderholz; T. Coghen; N. Schmitz; K.L. Wernhard; W. Wittek; G. Corrigan; G. Myatt; D. Radojicic; B. Saitta; J. Wells
Abstract Distributions of the Feynman x variable have been determined for positive and negative pions in charged current neutrino-proton and antineutrino-proton reactions with hadronic energy W > 3 GeV and Bjorken x B > 0.1. The distributions have been corrected for experimental effects such as measurement errors, uncertainties in estimating the neutrino energy and particle misidentification. In the framework of the quark-parton model, the distributions yield information about the fragmentation of forward going u and d quarks and backward going uu and ud diquarks. Approximate Feynman scaling is observed for the invariant Feynman x F distributions. They can be fitted by a power law of the form (1 − | x F |) n as suggested by the dimensional counting rules. Simple isospin relations predicted by the quark-parton model are fulfilled. The fragmentation of diquarks is compared with that of protons into π ± .
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.
Nuclear Physics | 1982
H. Grässler; C. Geich-Gimbel; R. Settles; R. Pech; P. Schmid; N. Schmitz; R. Batley; W. Wittek; R. Schulte; P. Grossmann; H.H. Seyfert; D. Radojicic; M. Aderholz; D.R.O. Morrison; G. Myatt; A. Grant; D. Lanske; V.T. Cocconi; B. Nellen; H. Wachsmuth; B. Saitta; P.O. Hulth; K.L. Wernhard; E. Simopoulou; R.H. Giles; K. Böckmann; H. Saarikko; L. Pape; P. Bosetti
In a selected sample of 6770 charged current (CC) events of νp interactions with 〈Eν〉 = 43 GeV and 〈W〉 = 4.6 GeV, 359 K0, 180 Λ and 13 Λ have been observed, which corresponds to a corrected production rate at least one neutral strange particle in (17.4±0.8)% of the CC events. The ratio of the inclusive Λ to K0 production cross section is found to be 0.26±0.03. The number of CC events containing at least one K0 increases with increasing Eν and Q2, while the CC events containing at least one Λ remain practically constant. The fractions of the total hadronic energy carried by K0 and Λ are found to be approximately the same in νp as in ep and μp interactions. In the hadronic c.m.s., the K0 are produced mostly forwards, the Λ mostly backwards, with asymmetry parameters of +0.32±0.02 and −0.45±0.06, respectively. The total strange particle production cross section is estimated to be (25±4)% of the cross section for production of CC events with W>1.5 GeV and that for charm production (10±2)% of the CC cross section well above charm threshold (W>3 GeV). The production of the resonances K∗+ (890) and Σ+ (1385) has been observed. The production rate of K∗+ (890) is comparable to that of D∗+ (2009), above the corresponding thresholds.
Nuclear Physics | 1981
P. Allen; J. Blietschau; H. Grässler; D. Lanske; R. Schulte; H.H. Seyfert; K. Böckmann; C. Geich-Gimbel; T. P. Kokott; B. Nellen; R. Pech; H. Saarikko; P. Bosetti; P.O. Hulth; D.R.O. Morrison; L. Pape; C. Peyrou; P. Schmid; W.G. Scott; E. Simopoulou; A. Vayaki; M. Aderholz; N. Schmitz; R. Settles; K.L. Wernhard; W. Wittek; J.R. Batley; R. Giles; P. Grossmann; G. Myatt
Abstract An analysis of the transverse momentum distributions of secondary hadrons produced in neutrino-proton charged current interactions is presented. It is found thatparticles going forward in the hadronic c.m.s. have a different behaviour from those going backward. A rise of the average transverse momentum squared as a function of both the invariant mass of the hadronic system and the fractional energy carried by the hadron in the c.m. frame, is observed. The result is not in good agreement with the predictions of a QCD based model if the non-perturbative parts are forward-backward symmetric. Using events with no missing neutral particles in the final state the average primordial transverse momentum squared of the quark inside the nucleon is estimated to be ∼0.3 GeV 2 / c 2 .
Nuclear Physics | 1983
P. Bosetti; P. Fritze; H. Grässler; F.J. Hasert; R. Schulte; K. Schultze; C. Geich-Gimbel; B. Nellen; R. Pech; B. Wünsch; A. Grant; P.O. Hulth; D. R. O. Morrison; L. Pape; H. Wachsmuth; A. Vayaki; K.W.J. Barnham; R. Beuselinck; E.F. Clayton; D.B. Miller; M. M. Mobayyen; A. Petrides; C. Albajar; G. Myatt; B. Saitta; J. Wells; T. Bolognese; D. Vignaud
Abstract The ratios of neutral current to charged current cross sections of neutrino and antineutrino interactions in heavy Ne/H 2 mixture have been measured in BEBC. The beam was the CERN SPS 200 GeV/ c narrow band beam. The ratios were obtained using a cut in the transverse momentum of the hadronic system. In the standard Glashow-Salam-Weinberg model, our results correspond to the value of sin 2 θ w = 0.182 ± 0.020 ± 0.012. By combining this experiment with data from a hydrogen target the coupling constants u L 2 and L 2 are found to be 0.15 ± 0.04 and 0.19 ± 0.05, respectively.
Nuclear Physics | 1981
H. Deden; P. Fritze; H. Grässler; F.J. Hasert; J. Morfin; R. Schulte; K. Böckmann; C. Geich-Gimbel; T. P. Kokott; B. Nellen; R. Pech; H. Saarikko; P. Bosetti; D. Cundy; A. Grant; P.O. Hulth; L. Pape; W.G. Scott; O. Skjeggestad; M. Mermikides; E. Simopoulou; A. Vayaki; K.W.J. Barnham; I. Butterworth; J.S. Chima; E.F. Clayton; D.B. Miller; M. M. Mobayyen; C. Penfold; K.J. Powell
The average transverse momentum squared, 〈p⊥2〉, of hadrons is studied as a function of W2 and of Q2 for ν and ν interactions on an isoscalar target. An increase of 〈p⊥2〉 with W2 is observed for the hadrons emitted forward in the hadronic c.m.s. The p⊥ dependence of the fragmentation function is found to factorise from the structure function at fixed W, but does not factorise at fixed Q2. Unlike the case of forward-going particles, the 〈p⊥2〉 of hadrons going backward in the c.m.s. shows no strong dependence on W2.
Nuclear Physics | 1987
M. Talebzadeh; J. Guy; W. Venus; M. Aderholz; K.W.J. Barnham; P. Bostock; E.F. Clayton; A. M. Cooper-Sarkar; M.L. Faccini-Turluer; H. Grässler; K. Hultquist; P. O. Hulth; H. Kreutzmann; J. Krstic; D.B. Miller; M. M. Mobayyen; G. Myatt; B. Nellen; Michael Andrew Parker; N. Schmitz; S. Sewell; E. Simopoulou; A. Vayaki; D. Vignaud; H. Wachsmuth; W. Wittek; B. Wünsch
Abstract A novel and efficient kinematic method is used to estimate the number of ν τ charged current interactions with E ν > 20 GeV in the BEBC beam dump experiment. The result, −14±12 ν τ events, is consistent with zero. The ratio of D s to D meson production in 400 GeV proton interactions in copper is estimated to be below 0.65 at 90% c.l. The oscillation probability P ( ν e → ν τ ) averaged over the electron-(anti)neutrino spectrum is found to be below 18%. The hypothesis that ν e and ν τ are identical is excluded by about 6 standard deviations. A remarkable event is described: it contains a muon, a high p T photon and a high p T hadron.
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
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.