Final data measured with the EMC forward spectrometer are presented on the production of forward charged hadrons in mu-p and mu-d scattering at incident beam energies between 100 and 280 GeV. The large statistic of 373000 events allows a study of the semi-inclusive hadron production as a function of z, p(T)2 and <p(T)2> in small Q2, x(Bj) and W bins. Charge multiplicity ratios and differences as a function of z and x(Bj) are given for p, d and n-targets. From the differences of charge multiplicities the ratio of the valence quark distributions of the proton d-upsilon(x)/u-upsilon(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 almost-equal-to 0.286. The measured sum corresponds to an absolute value of the ratio of the d and u quark charge of 0.44 +/- 0.10 stat. +/- 0.08 syst.

Forward Produced Hadrons In Mu-p and Mu-d Scattering and Investigation of the Charge Structure of the Nucleon

PERONI, Cristiana;
1991-01-01

Abstract

Final data measured with the EMC forward spectrometer are presented on the production of forward charged hadrons in mu-p and mu-d scattering at incident beam energies between 100 and 280 GeV. The large statistic of 373000 events allows a study of the semi-inclusive hadron production as a function of z, p(T)2 and in small Q2, x(Bj) and W bins. Charge multiplicity ratios and differences as a function of z and x(Bj) are given for p, d and n-targets. From the differences of charge multiplicities the ratio of the valence quark distributions of the proton d-upsilon(x)/u-upsilon(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 almost-equal-to 0.286. The measured sum corresponds to an absolute value of the ratio of the d and u quark charge of 0.44 +/- 0.10 stat. +/- 0.08 syst.
1991
52
361
387
DEEP INELASTIC-SCATTERING; STRUCTURE FUNCTIONS F2N; EXCLUSIVE RHO-0 PRODUCTION; PROTON STRUCTURE FUNCTIONS; TRANSVERSE-MOMENTUM; FRAGMENTATION FUNCTIONS; FINAL-STATES; AZIMUTHAL DISTRIBUTIONS; E+E-INTERACTIONS; JET PRODUCTION; EMC
J. ASHMAN;B. BADELEK;G. BAUM;J. BEAUFAYS;C. P. BEE;C. BENCHOUK;I. G. BIRD;S. C. BROWN;M. C. CAPUTO;H. W. K.;J. S. CHIMA;J. CIBOROWSKI;R. CLIFFT;G. COIGNET;F. COMBLEY;G. COURT;G. DAGOSTINI;J. DREES;M. DUREN;N. DYCEW;A. W. EDWARDS;M. EDWARDS;T. ERNST;J. FAVIER;M. I. FERRERO;D. FRANCIS;E. GABATHULER;R. GAMET;V. GIBSON;J. GILLIES;P. GRAFSTROM;K. HAMACHER;D. VONHARRACH;P. HAYMAN;J. R. HOLT;V. W. HUGHES;A. JACHOLKOWSKA;T. JONES;E. M. KABUSS;B. KORZEN;U. KRUNER;S. KULLANDER;U. LANDGRAF;D. LANSKE;D. LAUTERJUNG;F. LETTENSTROM;T. LINDQVIST;J. LOKEN;M. MATTHEWS;Y. MIZUNO;K. MONIG;F. MONTANET;E. NAGY;J. NASSALSKI;T. NIINIKOSKI;P. R. NORTON;F. G. OAKHAM;R. F. OPPENHEIM;A. M. OSBORNE;V. PAPAVASSILIOU;N. PAVEL;C. PERONI;H. PESCHEL;R. PIEGAIA;B. PIETRZYT;U. PIETRZYK;B. POVH;P. RENTON;J. M. RIEUBLAND;K. RITH;E. RONDIO;L. ROPELEWSKI;D. SALMON;A. SANDACZ;A. SCHLAGBOHMER;A. SCHNEIDER;T. SCHRODER;K. P. SCHULER;K. SCHULTZE;T. A. SHIBATA;T. SLOAN;A. STAIANO;H. E. STIER;J. STOCK;G. N. TAYLOR;J. C. THOMPSON;T. WALCHER;J. TOTH;L. URBAN;L. URBAN;H. WAHLEN;W. WALLUCKS;M. WHALLEY;S. WHEELER;W. S. C.;S. J. WIMPENNY;R. WINDMOLDERS;J. WOMERSLEY;K. ZIEMONS
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/110332
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