M. Crozon
Collège de France
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European Physical Journal A | 1983
J. Badier; J. Boucrot; J. Bourotte; G. Burgun; O. Callot; Ph. Charpentier; M. Crozon; D. Decamp; P. Delpierre; B. Gandois; R. Hagelberg; M. Hansroul; Y. Karyotakis; W. Kienzle; P. Le Du; J. Lefrancois; Th. Leray; J. Maillard; A. Michelini; P. Miné; G. Rahal; O. Runolfsson; P. Siegrist; A. Tilquin; J. Timmermans; J. Valentin; S. Weisz
A detailed study ofJ/ψ hadronic production has been performed in a high statistics experiment (more than 1.5 106J/ψ observed in their dimuon decay mode). Data have been taken with incident π±,K±,p±, on hydrogen and platinum targets, at 150, 200 and 280 GeV/c. We find from the observed nuclear dependance of the cross sections, that about 18% of theJ/ψ are produced diffractively. Using known structure functions of the quarks in the nucleon and in the pion, we derive estimations for the gluon structure functions.
European Physical Journal C | 1983
J. Badier; J. Bourotte; P. Miné; R. Vanderhaghen; S. Weisz; J. Boucrot; O. Callot; D. Decamp; Y. Karyotakis; J. Lefrancois; G. Burgun; P. Charpentier; B. Gandois; P. Le Du; G. Rahal; P. Siegrist; M. Crozon; P. Delpierre; Th. Leray; J. Maillard; A. Tilquin; Jérôme Valentin; R. Hagelberg; M. Hansroul; G. Matthiae; A. Michelini; O. Runolfsson; J.J.M. Timmermans
We have studied high statistics samples of dimuon events (∼35,000) produced from π± on platinum target in the mass interval 4.2≦Mμμ≦8.5 GeV at 150, 200 and 280 GeV/c. The π structure function is obtained by a fit ofd2σ/dx1dx2 to π+ and π− data. At 200 GeV, the simultaneous use of π+ and π− data allows a separate determination of the valence and sea structure functions of the π. Furthermore, the 150 and 280 GeV data allow an accurate determination of the shape of the valence structure function and give an estimate of its evolution betweenQ2=25 and 50 GeV2.
Physics Letters B | 1982
J. Badier; G. Burgun; O. Callot; J. Valentin; J. Bourotte; P. Charpentier; M. Crozon; G. Rahal; Th. Leray; P. Siegrist; S. Weisz; Y. Karyotakis; R. Hagelberg; A. Tilquin; P. Le Du; J. Lefrancois; M. Hansroul; O. Runolfsson; P. Miné; R. Vanderhaghen; B. Gandois; J. Boucrot; A. Michelini; P. Delpierre; D. Decamp; J. Maillard; W. Kienzle
From the analysis of multimuon events produced by π− interactions at 150 and 280 GeV/c in the NA3 spectrometer, we present evidence for the production of two J/ψ mesons in the same interaction (13 events seen, for an expected background of about 0.2 events). Some possible production mechanisms are described and an estimation of the cross section is given.
Physics Letters B | 1979
J. Badier; J. Boucrot; G. Burgun; O. Callot; Ph. Charpentier; M. Crozon; D. Decamp; P. Delpierre; B. Gandois; R. Hagelberg; M. Hansroul; W. Kienzle; P. Le Du; J. Lefrancois; Th. Leray; G. Matthiae; A. Michelini; P. Miné; O. Runolfsson; P. Siegrist; J. Timmermans; J. Valentin; R. Vanderhaghen; S. Weisz
Abstract We have measured the absolute cross section for dimuon production in hadron collisions at 200 GeV/c in the continuum region M = 4–8.5 GeV. In all the channels studied (pN, p N, π±N and π−H2) the experimental cross section is significantly larger by a factor of 2.3 ± 0.5 than expected from the Drell-Yan model. Furthermore, our proton-nucleon data allow a determination of the nucleon valence structure function which agrees with the deep inelastic lepton scattering data.
Physics Letters B | 1980
J. Badier; J. Boucrot; J. Bourotte; G. Burgun; O. Callot; Ph. Charpentier; M. Crozon; D. Decamp; P. Delpierre; P. Espigat; B. Gandois; R. Hagelberg; M. Hansroul; J. Karyotakis; W. Kienzle; P. Le Du; J. Lefrancois; Th. Leray; J. Maillard; G. Matthiae; A. Michelini; P. Miné; G. Rahal; O. Runolfsson; P. Siegrist; A. Tilquin; J. Timmermans; J. Valentin; R. Vanderhagen; S. Weisz
Abstract The first measurement of the kaon to pion structure function ratio has beenperformed in a high integrated luminosity experiment studying the production of massive muon pairs. The ratio u K u π clearly deviates from 1 for values of x1 > 0.7. A theoretical model comparison is also briefly discussed.
Physics Letters B | 1985
J. Badier; J. Bourotte; P. Miné; R. Vanderhaghen; S. Weisz; J. Boucrot; O. Callot; D. Decamp; Y. Karyotakis; J. Lefrancois; G. Burgun; P. Charpentier; B. Gandois; P. Le Du; G. Rahal; P. Siegrist; M. Crozon; P. Delpierre; Th. Leray; A. Tilquin; R. Hagelberg; M. Hansroul; A. Michelini; O. Runolfsson
Abstract From a study of multimuon events obtained in a high luminosity proton-platinum experiment at 400 GeV/ c , we find 5 ± 4 ψψ events, which correspond to a production cross section σ ( ψψ = 27 ± 10 pb. The observed production is compared to the ψψ events previously found in the same apparatus from incoming π − ; a comparison with QCD predictions is performed, giving a good agreement with expectations from gluon-gluon fusion. Finally, using like-sign dimuon, trimuon and quadrimuon events, we give model-dependent upper limits on beauty meson production: 2 nb/nucleon for central models, 20 nb/nucleon for diffractive production.
Physics Letters B | 1981
G. Burgun; Philippe Charpentier; R. Hagelberg; M. Crozon; P. Delpierre; P. Espigat; J. Badier; J. Bourotte; J. Boucrot; O. Callot
Abstract We present the final analysis of the nuclear effects on the cross section of dimuon production, using simultaneously a hydrogen and a platinum target in a 150, 200 and 280 GeV pion beam. For the dimuon mass interval 4.1 to 8.5 GeV, the ratio of the cross sections is in agreement with the Drell-Yan model within a 10% error, mainly due to systematics. The variation of this ratio with the dimuon mass, x 1 and x 2 is also in good agreement, and no variation with the transverse momentum is observed.
Physics Letters B | 1991
P. Abreu; W. Adam; F. Adami; T. Adye; T. P. A. Åkesson; P. Allen; S. Almehed; F. Alted; B. Åsman; Pierre Astier; A. Augustinus; F. Barao; G. Barbiellini; A. Baroncelli; O. Barring; W. Bartl; M. Baubillier; M. Begalli; I. Belokopytov; P. Beltran; D. Benedic; M. Berggren; D. Bertrand; S. Biagi; F. Bianchi; P. Billoir; D. Bloch; D. Bollini; T. Bolognese; M. Bonapart
Abstract In four-jet events from e+e− →Z0 →multihadrons one can separate the three principal contributions from the triple-gluon vertex, double gluon-bremsstrahlung and the secondary quark-antiquark production, using the shape of the two-dimensional angular distributions in the generalized Nachtmann-Reiter angle θ NR ∗ and the opening angle of the secondary jets. Thus one can identify directly the contribution from the triple-gluon vertex without comparison with a specific non-QCD model. Applying this new method to events taken with the DELPHI-detector we get for the ratio of the colour factor Nc to the fermionic Casimir operator C F : N c C F = 2.55 ± 0.55 ( stat. ) ± 0.4 ( fragm. + models ) ± 0.2 ( error in bias ) in agreement with the value 2.25 expected in QCD from Nc=3 and C F = 4 3 .
Physics Letters B | 1991
L. Knudsen; Jean-Pierre Koutchouk; Massimo Placidi; R. Schmidt; M. Crozon; J. Badier; A. Blondel; B. Dehning
Abstract The results of beam polarization measurements performed in 1990 at the CERN Large Electron Positron storage ring (LEP) are reported. A significant asymmetry was observed in the Compton back-scattered photon distribution when illuminating the LEP electron beam with circularly polarized laser light. The corresponding polarization level is estimated to be 9.1% ± 0.3% (statistical) ± 1.8% (systematic). The validity of the polarization signal was assessed by varying the laser light polarization and by applying to the electron beam known depolarizing resonances. The measurement is consistent with the predicted polarization degree.
Physics Letters B | 1992
L. Arnaudon; L. Knudsen; Jean-Pierre Koutchouk; R. Olsen; Massimo Placidi; R. Schmidt; M. Crozon; A. Blondel; R. Aβmann; B. Dehning
Abstract A transverse beam polarization of around 10% reproducibly observed in LEP in 1991. Resonant spin depolarization was performed at four occasions, from September 16 to November 11, providing measurements of the beam energy with a precision of ± 1.5 × 10−5. Several cross-checks were performed to ascertain that the observed resonance corresponds to the fundamental spin precession frequency. The variability of the results, ± 6 × 10−5, is consistent with the expected stability and reproducibility of the machine.