M. Bourquin
University of Geneva
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Featured researches published by M. Bourquin.
European Physical Journal A | 1983
M. Bourquin; R. M. Brown; Y. Chatelus; J. C. Chollet; A. Degré; Daniel Froidevaux; A. R. Fyfe; J. M. Gaillard; C. N. P. Gee; W. M. Gibson; R. J. Gray; P. Igo-Kemenes; P.W. Jeffreys; B. Merkel; R. Morand; R. J. Ott; H. Plothow; J. P. Repellin; B.J. Saunders; G. Sauvage; B. Schiby; H.-W. Siebert; V. J. Smith; K.-P. Streit; R. Strub; J.J. Thresher
Results on five different hyperon semileptonic decays from the WA2 experiment, performed in the CERN SPS charged hyperon beam, have been analysed within the framework of the Cabibbo model. For the first time, the inconsistencies, which inevitably occur when the results from different experiments are combined, have been avoided in these comprehensive fits to high statistics data from a single hyperon decay experiment. Excellent agreement with the basic Cabibbo model has been obtained using the WA2 data either alone or together with neutron lifetime measurements. These results contrast strongly with other recent Cabibbo analyses which have indicated the presence ofSU(3) breaking effects. Including radiative corrections we have obtained the results,F=0.477±0.012,D=0.756±0.011 and sinθc=0.231±0.003. The ratio (D/D+F) is 0.613±0.009, which is close to theSU(6) prediction of 3/5. Using additional information onft values for superallowed nuclear Fermi transitions, an upper limit on the mixing parameter sinθ3 in the Kobayashi-Maskawa six quark scheme has been obtained: |sinθ3|<0.20.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1991
P. Bene; M. Bourquin; J.H. Field; G. Forconi; A. Leger; J. Perrier; N. Produit; J.P. Richeux
Abstract A first-level charged particle trigger based on parallel processing and look-up tables has been developed for the L3 detector. It processes analog signals generated by the central tracking detector, a drift chamber with axial wires. The trigger decision is made on the total number of tracks, the number of coplanar pairs of tracks, or on more complicated topologies found in the projection normal to the beam axis. The system is very flexible and can be adjusted to a wide range of background conditions and tracking chamber efficiencies.
Nuclear Physics | 1979
M. Bourquin; R. M. Brown; Y. Chatelus; J.C. Chollet; M. Croissiaux; A. Degré; M. Ferro-Luzzi; Daniel Froidevaux; A. R. Fyfe; Jean-Marc Gaillard; C. N. P. Gee; W. M. Gibson; R.J. Gray; P. Igo-Kemens; P.W. Jeffreys; B. Merkel; R. Morand; R.J. Ott; H. Plothow; J.-P. Repellin; B.J. Saunders; G. Sauvage; B. Schiby; H.-W. Siebert; V. J. Smith; K.-P. Streit; R. Strub; J.J. Thresher; J. Trischuk
Abstract A charge hyperon beam has been brought into operation at the CERN SPS. Particles are identified by a DISC Cerenkov counter, and decay products are analysed by a magnetic spectrometer. Cross sections for the inclusive production of π + , K + , p , Σ + , Σ − , ζ − , d, and π − , K − , p , Σ + , Σ − , ζ − , ω − , d in the forward direction have been measured at laboratory momenta between 70 and 130 GeV/ c . This range of momenta corresponds to 0.35 ⩽ x ⩽ 0.66 for an incident proton momentum of 200 GeV/ c . Antihyperon ( Σ − , ζ − , Σ + ) and Σ + and ω − fluxes have been measured for the first time in a hyperon beam. Scaling behaviour is observed when the data are compared with the results from other experiments. The inclusive particle production cross sections have a (1 − x ) n dependence, where n is characteristics of the particle. A search has been made for new particles in the mass range 2–10 GeV/ c 2 . No evidence is found for such particles.
Physics Letters B | 1983
S. F. Biagi; M. Bourquin; A.J. Britten; R. M. Brown; H. J. Burckhart; A.A. Carter; Ch. Doré; P. Extermann; M. Gailloud; C. N. P. Gee; W. M. Gibson; J.C. Gordon; R. J. Gray; P. Igo-Kemenes; P. Jacot-Guillarmod; W. C. Louis; T. Modis; P. Muhlemann; Ph. Rosselet; B. J. Saunders; P. Schirato; H.-W. Siebert; V. J. Smith; K. P. Streit; J. J. Thresher; S.N. Tovey; R. Weill
Abstract A narrow state has been observed in the reaction Σ − + Be → ( Λ K − π + π + ) + X in an experiment at the CERN SPS hyperon beam. At 2.46 GeV/ c 2 the effective ( Λ K − π + π + ) mass distribution shows an excess of 82 events above a background estimated to be 147, corresponding to a statistical significance of more than 6 standard deviations. The positive charge of the observed final state, which has strangeness −2, suggests the interpretation as a Cabibbo favoured decay of the charmed strange baryon, A + [quark content (csu)]. The cross section times branching ratio is measured to be σ · B = (5.3 ± 2.0) μ b/ (Be nucleus) for x > 0.6. The invariant production cross section is described by E d 3 σ /d p 3 ∞ (1 - x ) (1.7±0.7) exp[−(1.1 −0.4 +0.7 ) p T 2 ].
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1987
J.A. Bakken; G. Bellomi; R. Bizzarri; T. Böhringer; B. Borgia; M. Bourquin; D. Boutigny; J.P. Burq; F. Carminati; M. Chemarin; P. Denes; C. Dionisi; H. Elmamouni; P. Extermann; S. Falciano; F. Ferroni; G. Gratta; J.T. He; B. Ille; P. Kaaret; P. Klok; P. Lebrun; E. Longo; Y.S. Lu; J.P. Martin; U. Micke; R. Morand; J. Ossman; D. Perret-Gallix; E. Perrin
Abstract A prototype of the L3 electromagnetic calorimeter to be used at LEP and consisting of 100 tapered BGO crystals has been tested in an electron beam in the energy range of 2 to 50 GeV. The energy resolution and linearity of response have been measured, and are compared to predictions made with the GEANT Monte Carlo program.
Physics Letters B | 1986
M. Bourquin; R. M. Brown; H. J. Burckhart; P. Extermann; M. Gailloud; W. M. Gibson; J.C. Gordon; P. Jacot-Guillarmod; Ph. Rosselet; P. Schirato; H.-W. Siebert; V. J. Smith; K. P. Streit; J. J. Thresher
Abstract Evidence for narrow states produced by Σ− interactions in beryllium, and decaying into ( Λ p + pions ), has been obtained in an experiment at the CERN SPS hyperon beam. At 3.1 GeV/c2, the ( Λ p π + π + ), ( Λ p π + π + π − ) and ( Λ p π + π − ) effective mass distributions show an excess of 45, 19 and 62 events above a background of 50, 28 and 187, respectively. The possibility that these three signals are statistical fluctuations is remote. The observed widths of the signals are compatible with the mass resolution of the apparatus, 24 MeV/c2 FWHM. We have not been able to find an interpretation of the quantum numbers of the final states, which are baryon number 0, strangeness −1 and charge +1, 0 and −1.
Physics Letters B | 1985
S. F. Biagi; M. Bourquin; A.J. Britten; R. M. Brown; H. J. Burckhart; A.A. Carter; Ch. Doré; P. Extermann; M. Gailloud; C. N. P. Gee; W. M. Gibson; J.C. Gordon; R. J. Gray; P. Igo-Kemenes; P. Jacot-Guillarmod; W. C. Louis; T. Modis; Ph. Rosselet; B. J. Saunders; P. Schirato; H.-W. Siebert; V. J. Smith; K. P. Streit; J. J. Thresher; S.N. Tovey; R. Weill
Abstract The lifetime of the charmed strange baryon A+ has been determined in an experiment at the CERN SPS hyperon beam from the distribution of distances between production and decay of A+ candidates of known momentum. The result is: τ = (4.8 −1.8 +2.9 ) × 10 −13 s .
Nuclear Physics | 1981
S. F. Biagi; M. Bourquin; A.J. Britten; R. M. Brown; H. J. Burckhart; A.A. Carter; J. R. Carter; Ch. Doré; P. Extermann; M. Gailloud; C. N. P. Gee; W. M. Gibson; J.C. Gordon; R. J. Gray; P. Igo-Kemenes; W. C. Louis; T. Modis; P. Muhlemann; J. Perrier; Ph. Rosselet; B. J. Saunders; P. Schirato; H.-W. Siebert; V. J. Smith; D. P. Stickland; K.-P. Streit; J. J. Thresher; R. Weill
The Σ− p and Σ− d total cross sections have been measured to a statistical accuracy of ±1% and ±0.5%, respectively, at five momenta from 74.5 to 136.9 GeV/c, using the hyperon beam at the CERN SPS. The Ξ−p and Ξ− d total cross sections have also been measured to the same statistical accuracy at 101.5 and 133.8 GeV/c. The systematic uncertainty at each momentum is estimated to be of the order of ±0.5%. The hyperon-nucleon cross sections are shown to be rising with energy, and the data are compared with various phenomenological models.
Physics Letters B | 1979
M. Bourquin; R. M. Brown; Y. Chatelus; J.C. Chollet; A. Degré; Daniel Froidevaux; A. R. Fyfe; Jean-Marc Gaillard; C. N. P. Gee; W. M. Gibson; P. Igo-Kemenes; P.W. Jeffreys; B. Merkel; R. Morand; H. Plothow; J.-P. Repellin; B.J. Saunders; G. Sauvage; B. Schiby; H.-W. Siebert; V. J. Smith; K.-P. Streit; R. Strub; J.J. Thresher; S.N. Tovey
Abstract In an experiment in the CERN-SPS charged-hyperon beam, the main Ω − decay branching ratios have been measured to be Γ(Ω − →Λ K − /Γ( all )=0.686±0.013 , Γ(Ω −1 →Ξ 0 π − )/Γ( all )=0.234±0.013 , Γ(Ω − →Ξ − π 0 )/Γ( all )=0.080±0.008 . The relative branching ratio of the two Ξπ modes provides a test of the ΔI= 1 2 rule in decuplet-octet transitions. A search has also been made for the rare decay modes Ω − →Λπ − , Ω − →Ξ − γ, Ω − →Ξ − π + π − and Ω − →Ξ 0 e − ν .
Physics Letters B | 1975
M. Bourquin; Jean-Marc Gaillard
Abstract The data on the dilepton spectra in a forward cone are used to predict the ϱ 0 , ω 0 , and ψ production at θ cm ≈ 90° and their contributions to the single lepton spectra. The π, (ϱ 0 +ω 0 ), and ψ inclusive cross-sections are well fitted over the entire p T range by a simple expression. Combined contributions from ϱ 0 , ω 0 , and ψ are found to account for about 30% of the observed lepton spectra. The contribution from the dilepton continuum is also discussed.