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Featured researches published by M.I. Ferrero.


Nuclear Physics | 1989

AN INVESTIGATION OF THE SPIN STRUCTURE OF THE PROTON IN DEEP INELASTIC SCATTERING OF POLARISED MUONS ON POLARISED PROTONS

Jg 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. Cibarowski; 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; R. Gamet; V. Gibson; J. Gillies; P. Grafström

An investigation of the spin structure of the proton in deep inelastic scattering of polarised muons on polarised protons


Physics Letters B | 1983

The ratio of the nucleon structure functions

J.J. Aubert; G. Bassompierre; X. De Bouard; C. Broll; G. Coignet; Y. Declais; J. Favier; M. Maire; H. Minssieux; P. Payre; H. Pessard; M. Schneegans; J.M. Thenard; L. Urban; C. Best; J. Carr; R.W. Clifft; M. Edwards; P. R. Norton; J. Thompson; F.W. Brasse; W. Flauger; J. Gayler; V. Gerhardt; C. Goessling; V. Korbel; R. Dobinson; U. Dosselli; A. Edwards; E. Gabathuler

Abstract Using the data on deep inelastic muon scattering on iron and deuterium the ratio of the nucleon structure functions F 2 N ( Fe )/ F 2 N ( D ) is presented. The observed x -dependence of this ratio is in disagreement with existing theoretical predictions.


Nuclear Physics | 1997

F^N_2

M. Arneodo; A. Arvidson; B. Badelek; M. Ballintijn; G. Baum; J. Beaufays; I. Bird; P. Björkholm; Michiel Botje; C. Broggini; W. Brückner; A. Brüll; Wj Burger; J. Ciborowski; R. van Dantzig; A. Dyring; H. Engelien; M.I. Ferrero; L. Fluri; U. Gaul; T. Granier; M. Grosse-Perdekamp; D. von Harrach; M. van der Heijden; C. A. Heusch; Q. Ingram; M. de Jong; E. Kabuß; R. Kaiser; T. Ketel

The muon-proton and muon-deuteron inclusive deep inelastic scattering cross sections were measured in the kinematic range 0.002 < x < 0.60 and 0.5 < Q(2) < 75 GeV2 at incident muon energies of 90, 120, 200 and 280 GeV. These results are based on the full data set collected by the New Muon Collaboration, including the data taken with a small angle trigger. The extracted values of the structure functions F-2(p) and F-2(d) are in good agreement with those from other experiments. The data cover a sufficient range of y to allow the determination of the ratio of the longitudinally to transversely polarised virtual photon absorption cross sections, R = sigma(L)/sigma(T), for 0.002 < x < 0.12. The values of R are compatible with a perturbative QCD prediction; they agree with earlier measurements and extend to smaller x.The muon-proton and muon-deuteron inclusive deep inelastic scattering cross sections were measured in the kinematic range 0.002<x<0.60 and 0.5<Q2<75 GeV2 at incident muon energies of 90, 120, 200 and 280 GeV. These results are based on the full data set collected by the New Muon Collaboration, including the data taken with a small angle trigger. The extracted values of the structure functions F2p and F2d are in good agreement with those from other experiments. The data cover a sufficient range of y to allow the determination of the ratio of the longitudinally to transversely polarised virtual photon absorption cross sections, R= sigma(L)/sigma(T), for 0.002<x<0.12 . The values of R are compatible with a perturbative QCD prediction; they agree with earlier measurements and extend to smaller x.


Physics Letters B | 1992

for iron and deuterium

P. Amaudruz; M. Arneodo; C. Scholz; G. van Middelkoop; H. Engelien; F. Klein; S. Kullander; J.-L. Vuilleumier; U. Krüner; T. Walcher; F. Sever; R. van Dantzig; J. Domingo; R. Schumacher; U. Landgraf; C.H.Quentin Ingram; U. Sennhauser; A. Staiano; M. van der Heijden; M.I. Ferrero; C. Mariotti; D. Nowotny; K. Rith; A. Sandacz; R. Rieger; K. Kurek; J. Drinkard; N. Pavel; A. Brüll; R. Windmolders

The structure functions F2p and F2d measured by deep inelastic muon scattering at incident energies of 90 and 280 GeV are presented. These measurements cover a large kinematic range, 0.006 less-tha ...


Nuclear Physics | 1985

Measurement of the proton and deuteron structure functions, F2p and F2d, and of the ratio sigmaL/sigmaT.

J.J. Aubert; G. Bassompierre; K.H. Becks; C. Best; E. Böhm; X. De Bouard; F.W. Brasse; C. Broll; S. Brown; J. Carr; R.W. Clifft; J.H. Cobb; G. Coignet; F. Combley; G. D'Agostini; W.D. Dau; J.K. Davies; Y. Declais; R. Dobinson; U. Dosselli; J. Drees; A. Edwards; M. Edwards; J. Favier; M.I. Ferrero; W. Flauger; E. Gabathuler; R. Gamet; J. Gayler; V. Gerhardt

Abstract The x and Q 2 dependence of the single photon exchange cross section d 2 σ /d Q 2 d x and the proton structure functions F 2 ( x , Q 2 ) and R ( x , Q 2 ) have been measured in deep inelastic muon proton scattering in the region 0.02 x Q 2 2 . By comparing data at different incident muon energies R was found to have little kinematic dependence and an average value of −0.010 ± 0.037 (stat.) ± 0.102 (stat.). The observed deviations from scaling gave the value of Λ MS , the QCD mass scale parameter, to be 105 −45 +55 (stat.) −45 +85 (syst.) MeV. The fraction of the momentum of the nucleon carried by gluons was found to be ∼56% at Q 2 ∼22.5 GeV 2 . It is shown that to obtain a description of the data for F 2 ( x , Q 2 ) together with that measured in deep inelastic electron-proton scattering at lower Q 2 it is necessary to include additional higher twist contributions. The value of Λ MS remains unchanged with the inclusion of these contributions which were found to have an x -dependence of the form x 3 /(1 − x ).


Physics Letters B | 1995

Proton and deuteron F2 structure functions in deep inelastic muon scattering

M. Arneodo; A. Arvidson; B. Badelek; M. Ballintijn; G. Baum; J. Beaufays; I.G. Bird; P. Björkholm; M. Botje; C. Broggini; W. Brückner; A. Brüll; W.J. Burger; J. Ciborowski; R. van Dantzig; A. Dyring; H. Engelien; M.I. Ferrero; L. Fluri; U. Gaul; T. Granier; M. Grosse-Perdekamp; D. von Harrach; M. van der Heijden; C. A. Heusch; G. Igo; Q. Ingram; M. de Jong; E.M. Kabuß; R. Kaiser

The proton and deuteron structure functions F2p and F2d were measured in the kinematic range 0.006<x<0.6 and 0.5<Q^2<75 GeV^2, by inclusive deep inelastic muon scattering at 90, 120, 200 and 280 GeV. The measurements are in good agreement with earlier high precision results. The present and earlier results together have been parametrised to give descriptions of the proton and deuteron structure functions F2 and their uncertainties over the range 0.006<x<0.9.The proton and deuteron structure funtions F2p and F2d were measured in the kinematic range 0.006 < x < 0.6 and 0.5 < Q2 < 75 GeV2, by inclusive deep inelastic muon scattering at 90, 120, 200 and 280 GeV. The measurements are in good agreement with earlier high precision results. The present and earlier results together have been parametrised to give descriptions of the proton and deuteron structure functions F2 and their uncertainties over the range 0.006 < x < 0.9.


Nuclear Physics | 1983

A Detailed Study of the Proton Structure Functions In Deep Inelastic Muon-proton Scattering

J.J. Aubert; P. Payre; E. Gabathuler; P.J. Hayman; G. Coignet; W.S.C. Williams; W.D. Dau; C. Gössling; P. Gregory; F.W. Brasse; K.H. Becks; M. Villers; U. Landgraf; R. Dobinson; J. Gayler; Hugh E. Montgomery; M. Schneegans; J. Haas; G. D'Agostini; P. Dalpiaz; J.M. Crespo; W. Stockhausen; R. Gamet; K. Rith; M. Henckes; M. Maire; A.M. Osborne; C. Best; L. Massonnet; J. McNicholas

Abstract Dimuon and trimuon events produced by the interaction of 250 GeV muons in an iron target have been studied and are shown to originate predominantly from charm production. The data are used to measure the contribution of charm to the nucleon structure function F 2 . The cross sections for real photoproduction ( Q 2 =0) of charm in the current fragmentation region are derived as a function of photon energy and are found to be ∼0.6% of the total, hadronic photoproduction cross section in this energy range. The measured cross sections are found to be well represented by the photon-gluon fusion model. The charmed quark fragmentation function is obtained by using this model to fit the measured decay muon energy distribution and is found to be well represented by exp(1.6±1.6) Z . The data are used to study the momentum distribution of the gluons in the nucleon. An upper limit of 1.4% (90% confidence level) is set on the branching ratio D→ μν and a model-dependent upper limit on the branching ratio F→ μν is derived.


Nuclear Instruments and Methods | 1981

Measurement of the proton and the deuteron structure functions, F2p and F2d

O.C. Allkofer; J.J. Aubert; G. Bassompierre; K.H. Becks; Y. Bertsch; C. Besson; C. Best; E. Böhm; D.R. Botterill; F.W. Brasse; C. Broll; J. Carr; B. Charles; R.W. Clifft; J.H. Cobb; G. Coignet; F. Combley; J.M. Crespo; P. Dalpiaz; W.D. Dau; J.K. Davies; Y. Declais; R. Dobinson; J. Drees; A. Edwards; M. Edwards; J. Favier; M.I. Ferrero; J.H. Field; W. Flauger

Abstract The European Muon Collaboration has built a large magnetic spectrometer system for deep inelastic muon scattering experiments at the CERN SPS muon beam. The general characteristics of the apparatus — composed of a target of either liquid hydrogen or deuterium, or iron plus scintillator, followed by a large magnet with wire chambers before and after it for precise angle and momentum measurement, a muon identifier, large trigger hodoscopes, and hadron identifiers — are explained and each part is described in some detail. The main features of the data-acquisition and apparatus-monitoring systems and of the off-line event reconstruction are given.


European Physical Journal C | 1991

Production of charmed particles in 250 GeV μ+-iron interactions

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. Dyce; A. Edwards; M. Edward; T. Ernst; M.I. Ferrero; D. Francis; E. Gabathuler; R. Gamet; V. Gibson; J. Gillies; P. Grafström

Differential multiplicities of forward produced hadrons in deep inelastic muon scattering on nuclear targets have been compared with those from deuterium. The ratios are observed to increase towards unity as the virtual photon energy increases with no significant dependence on the other muon kinematic variables. The hadron transverse momentum distribution is observed to be broadened in nuclear targets. The dependence on the remaining hadron variables is investigated and the results are discussed in the framework of intranuclear interaction models and in the context of the EMC effect.


Nuclear Physics | 1995

A large magnetic spectrometer system for high-energy muon physics

M. Arneodo; A. Paic; C. Scholz; G. van Middelkoop; H. Engelien; Y. Tzamouranis; F. Klein; A. Witzmann; S. Kullander; J.-L. Vuilleumier; E. Rondio; H.J. Kessler; T. Walcher; F. Sever; R. van Dantzig; G.K. Mallot; U. Landgraf; C. Whitten; A. Mücklich; C.H.Quentin Ingram; D. Sanders; R. Windmolders; M. van der Heijden; M.I. Ferrero; A. Milsztajn; C. Mariotti; D. Nowotny; K. Rith; A. Sandacz; R. Rieger

We present the structure function ratios F2(Li)/F2(D) and F2(C)/F2(D) measured in deep inelastic muon-nucleus scattering at a nominal incident muon energy of 200 GeV. The kinematic range 0.0001 s x s 0.7 and 0.01 s Q˜2 s 70 GeV˜2 is covered. For values of

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C. Broll

Laboratoire d'Annecy-le-Vieux de physique des particules

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K.H. Becks

University of Wuppertal

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R.W. Clifft

Rutherford Appleton Laboratory

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