J. M. Rieubland
CERN
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Featured researches published by J. M. Rieubland.
Physics Letters B | 1993
H. Bøggild; J. Boissevain; M. Cherney; J. Dodd; J. Downing; S. Esumi; Christian Fabjan; A. Franz; K.H. Hansen; T. Humanic; T. Ikemoto; B. V. Jacak; H. Kalechofsky; T. Kobayashi; R. Kvatadze; Y.Y. Lee; M. Leltchouk; B. Lörstad; N. Maeda; Y. Miake; A. Miyabayashi; M. Murray; S. Nagamiya; S. Nishimura; S.U. Pandey; F. Piuz; V. Polychronakos; M. Potekhin; G. Poulard; D. Rahm
Abstract π + π + correlations from S + Pb collisions at 200 GeV/ c per nucleon, measured by the focusing spectrometer of the NA44 experiment at CERN, are presented. The large data set, particularly at small values of Q inv , allows determination of the detailed shape of the correlation function. We construct the background by event mixing, and correct for resolution, Coulomb interaction, and distortion of single-particle spectra which produce effects large compared to the statistical errors at small Q inv . An exponential, rather than gaussian, source distribution is slightly favoured, but both are statistically acceptable.
Physics Letters B | 1988
R. Kunne; C.I. Beard; R. Birsa; Kors Bos; F. Bradamante; D.V. Bugg; A.S. Clough; S. Dallatorre-Colautti; S. Degli-Agosti; J.A. Edgington; J.R. Hall; E. Heer; R. Hess; J.C. Kluyver; C. Lechanoine-Leluc; L. Linssen; A. Martin; T. Niinikoski; Y. Onel; Aldo Penzo; D. Rapin; J. M. Rieubland; A. Rijllart; P. Schiavon; R.L. Shypit; F. Tessarotto; A. Villari; P. Wells
Abstract Asymmetries A 0 n have been measured at LEAR for s ¯ s elastic scattering for 15 beam momenta from 497 to 1550 MeV/ c .
European Physical Journal C | 1993
J.G. Ashman; B. Badelek; Günter Baum; J. Beaufays; C. P. Bee; C. Benchouk; I. Bird; S. Brown; M. C. Caputo; H. W. K. Cheung; J. S. Chima; J. Ciborowski; R.W. Clifft; G. Coignet; F. Combley; G.R. Court; G. D'Agostini; J. Drees; M. Düren; N. Dyce; A. Edwards; M. Edwards; T. Ernst; M.I. Ferrero; D. Francis; E. Gabathuler; J. Gajewski; R. Gamet; V. Gibson; J. Gillies
Results are presented on the ratios of the nucleon structure function in copper to deuterium from two separate experiments. The data confirm that the nucleon structure function,F2, is different for bound nucleons than for the quasi-free ones in the deuteron. The redistribution in the fraction of the nucleons momentum carried by quarks is investigated and it is found that the data are compatible with no integral loss of quark momenta due to nuclear effects.
European Physical Journal C | 1991
J.G. Ashman; B. Badelek; Günter Baum; J. Beaufays; C. P. Bee; C. Benchouk; I.G. Bird; S. Brown; M. C. Caputo; H. W. K. Cheung; J. S. Chima; J. Ciborowski; R.W. Clifft; G. Coignet; F. Combley; G.R. Court; G. D'Agostini; J. Drees; M. Düren; N. Dycew; A. Edwards; M. Edwards; T. Ernst; J. Favier; M.I. Ferrero; D. Francis; E. Gabathuler; R. Gamet; V. Gibson; J. Gillies
Final data measured with the EMC forward spectrometer are presented on the production of forward charged hadrons in μp and μd scattering at incident beam energies between 100 and 280 GeV. The large statistic of 373 000 events allows a study of the semi-inclusive hadron production as a function ofz,pT2 and 〈pT2〉 in smallQ2,xBj andW bins. Charge multiplicity ratios and differences as a function ofz andxBj are given forp, d andn-targets. From the differences of charge multiplicities the ratio of the valence quark distributions of the protondv(x)/uv(x) is determined for the first time in charged lepton scattering. The Gronau et al. sum rule is tested, the measured sum being 0.31±0.06 stat. ±0.05 syst., compared with the theoretical expectation of 2/7≈0.286. The measured sum corresponds to an absolute value of the ratio of thed andu quark charge of 0.44±0.10 stat.±0.08 syst.
Physics Letters B | 1999
H. Bøggild; J. Boissevain; J. Dodd; S. Esumi; Christian Fabjan; D. Ferenc; A. Franz; D. Hardtke; H. W. van Hecke; T. J. Humanic; T. Ikemoto; B.V. Jacak; H. Kalechofsky; T. Kobayashi; R. Kvatadze; Y.Y. Lee; M. Leltchouk; B. Lörstad; N. Maeda; Y. Miake; A. Miyabayashi; M. Murray; S. Nagamiya; S. Nishimura; G. Paić; S.U. Pandey; F. Piuz; V. Polychronakos; M. Potekhin; G. Poulard
Abstract π + π + π + correlations from sulphur-lead collisions at 200 GeV/c per nucleon are presented as measured by the focusing spectrometer of experiment NA44 at CERN. We have investigated the three-pion correlation function at mid-rapidity and found that a genuine three-body correlation is suppressed. A possible interpretation of this result is that the emission of particles is partially coherent.
Nuclear Physics | 1989
R. Kunne; C.I. Beard; R. Birsa; Kors Bos; F. Bradamante; D.V. Bugg; A.S. Clough; S. Dalla Torre-Colautti; J.A. Edgington; J.R. Hall; E. Heer; R. Hess; J.C. Kluyver; C. Lechanoine-Leluc; L. Linssen; A. Martin; Tapio Niinikoski; Y. Onel; Aldo Penzo; D. Rapin; J. M. Rieubland; A. Rijllart; P. Schiavon; R.L. Shypit; F. Tessarotto; A. Villari; P S Wells
Measurements have been made of the differential cross section and asymmetry Aon for pp elastic scattering at 15 incident momenta between 497 MeV/c and 1550 MeV/c. The angular range where both particles have enough energy to traverse target and setup has been covered. The results are compared with predictions of various NN potential models. None of these models fully explains the present results, although the general trend of the data is predicted correctly.
Physics Letters B | 1991
R.A. Kunne; C.I. Beard; R. Birsa; Kors Bos; F. Bradamante; D.V. Bugg; A.S. Clough; S. Dalla Torre-Colautti; J.A. Edgington; M. Giorgi; J.R. Hall; E. Heer; R. Hess; J.C. Kluyver; C. Lechanoine-Leluc; L. Linssen; A. Martin; T. Niinikoski; Y. Onel; Aldo Penzo; D. Rapin; J. M. Rieubland; A. Rijllart; P. Schiavon; R.L. Shypit; F. Tessarotto; A. Villari
Abstract The depolarization parameter D onon in p p elastic scattering has been measured at LEAR for thirteen momenta between 679 and 1550 MeV/c in the backward angular region. Striking disagreement with theoretical models is observed.
European Physical Journal C | 1992
J.G. Ashman; B. Badelek; Günter Baum; J. Beaufays; C. P. Bee; C. Benchouk; I. Bird; S. Brown; M. C. Caputo; H. W. K. Cheung; J. S. Chima; J. Ciborowski; R.W. Clifft; G. Coignet; F. Combley; G.R. Court; G. D'Agostini; J. Drees; M. Düren; N. Dyce; A. Edwards; M. Edwards; T. Ernst; M.I. Ferrero; D. Francis; E. Gabathuler; J. Gajewski; R. Gamet; V. Gibson; J. Gillies
Measurements are presented of the inclusive distributions of theJ/Ψ meson produced by muons of energy 200 GeV from an ammonia target. The gluon distribution of the nucleon has been derived from the data in the range 0.04<x<0.36 using a technique based on the colour singlet model. An arbitrary normalisation factor is required to obtain a reasonable integral of the gluon distribution. Some comments are made on the use ofJ/Ψ productionby virtual photons to extract the gluon distribution at HERA.
Nuclear Physics | 1994
H. Bøggild; J. G. Boissevain; M. Cherney; J. Dodd; J. Downing; Shinichi Esumi; C. Fabjan; D. E. Fields; A. Franz; K.H. Hansen; T. J. Humanic; T. Ikemoto; B. V. Jacak; R. Jayanti; H. Kalechofsky; T. Kobayashi; R. Kvatadze; Y.Y. Lee; M. Leltchouk; B. Lörstad; N. Maeda; A. Medvedev; Y. Miake; A. Miyabayashi; M. Murray; S. Nagamiya; S. Nishimura; E. Noteboon; S.U. Pandey; F. Piuz
Abstract We have measured π ± , K ± , P and P spectra from proton and sulfur collisions with nuclear targets at the at beam energies of 450 Gev and 200 Gev per nucleon respectively. For central SA collisions we see that kaons and (anti)protons have large transverse energies. Protons are moved into central rapidity by rescattering where they annhilate antiprotons. The RQMD event generator qualitatively reproduces these trends while Fritjof does not.
AIP Conf. Proc.; (United States) | 2008
R. Bernard; P. Chaumette; J. Derégel; R. Duthil; J. Fabre; C. Lesmond; G. Seité; Tapio Niinikoski; J. M. Rieubland; J. Ball; Ph. Chesny
A frozen spin target has been constructed at CEN‐Saclay for nucleon‐nucleon scattering experiments at the P.S. SATURNE II. The target which may have a maximum volume of 100 cm3 is cooled in a vertical dilution refrigerator. The magnet system is entirely super‐conducting and allows the polarization vector to be oriented in three orthogonal directions. This target has been already used for the measurements of several parameters in the p−p scattering.