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Polarised quark distributions in the nucleon from semi-inclusive spin asymmetries

  • B. Adeva*
  • , T. Akdogan
  • , E. Arik
  • , A. Arvidson
  • , B. Badelek
  • , G. Bardin
  • , G. Baum
  • , P. Berglund
  • , L. Betev
  • , R. Birsa
  • , N. de Botton
  • , F. Bradamante
  • , A. Bravar
  • , A. Bressan
  • , S. Bültmann
  • , E. Burtin
  • , D. Crabb
  • , J. Cranshaw
  • , T. Çuhadar
  • , S. Dalla Torre
  • R. van Dantzig, B. Derro, A. Deshpande, S. Dhawan, C. Dulya, S. Eichblatt, D. Fasching, F. Feinstein, C. Fernandez, S. Forthmann, B. Frois, A. Gallas, J. A. Garzon, H. Gilly, M. Giorgi, E. von Goeler, S. Goertz, G. Gracia, N. de Groot, M. Grosse Perdekamp, K. Haft, D. von Harrach, T. Hasegawa, P. Hautle, N. Hayashi, C. A. Heusch, N. Horikawa, V. W. Hughes, G. Igo, S. Ishimoto, T. Iwata, E. M. Kabuß, T. Kageya, A. Karev, H. J. Kessler, T. J. Ketel, J. Kiryluk, Y. Kisselev, D. Krämer, V. Krivokhijine, W. Kröger, V. Kukhtin, K. Kurek, J. Kyynäräinen, M. Lamanna, U. Landgraf, J. M. Le Goff, F. Lehar, A. de Lesquen, J. Lichtenstadt, M. Litmaath, A. Magnon, G. K. Mallot, F. Marie, A. Martin, J. Martino, T. Matsuda, B. Mayes, J. S. McCarthy, K. Medved, W. Meyer, G. van Middelkoop, D. Miller, Y. Miyachi, K. Mori, J. Moromisato, J. Nassalski, L. Naumann, T. O. Niinikoski, J. E.J. Oberski, A. Ogawa, C. Ozben, H. Pereira, F. Perrot-Kunne, D. Peshekhonov, L. Pinsky, S. Platchkov, M. Plo, D. Pose, H. Postma, J. Pretz, R. Puntaferro, G. Rädel, A. Rijllart, G. Reicherz, J. Roberts, M. Rodriguez, E. Rondio, B. Roscherr, I. Sabo, J. Saborido, A. Sandacz, I. Savin, P. Schiavon, A. Schiller, E. P. Sichtermann, F. Simeoni, G. I. Smirnov, A. Staude, A. Steinmetz, U. Stiegler, H. Stuhrmann, M. Szleper, F. Tessarotto, D. Thers, W. Tlaczala, A. Tripet, G. Unel, M. Velasco, J. Vogt, R. Voss, C. Whitten, R. Windmolders, R. Willumeit, W. Wislicki, A. Witzmann, J. Ylöstalo, A. M. Zanetti, K. Zaremba, J. Zhao
*Corresponding author for this work
  • University of Santiago de Compostela
  • Istanbul Technical University
  • Universite de Mons
  • Uppsala University
  • University of Warsaw
  • CEA Saclay
  • Bielefeld University
  • Aalto University
  • Ludwig Maximilian University of Munich
  • University of Trieste
  • Johannes Gutenberg University Mainz
  • CERN
  • University of Virginia
  • Delft University of Technology
  • University of California at Los Angeles
  • Yale University
  • CIEMAT
  • Fermi National Accelerator Laboratory
  • Northwestern University
  • University of Wisconsin
  • University of Houston
  • Helmholtz-Zentrum Hereon
  • University of Freiburg
  • Gammadata
  • Northeastern University
  • Ruhr University Bochum
  • National Institute for Subatomic Physics
  • SLAC National Accelerator Laboratory
  • Nagoya University
  • University of Miyazaki
  • Paul Scherrer Institute
  • RIKEN
  • University of California at Santa Cruz
  • High Energy Accelerator Research Organization, Tsukuba
  • University of Michigan, Ann Arbor
  • Joint Institute for Nuclear Research
  • Tel Aviv University
  • Pennsylvania State University
  • Rice University
  • Universidad de Buenos Aires
  • Warsaw University of Technology
  • F. Hoffmann-La Roche AG
  • Los Alamos National Laboratory

Research output: Contribution to journalArticlepeer-review

204 Citations (Scopus)

Abstract

We present a measurement of semi-inclusive spin asymmetries for positively and negatively charged hadrons from deep inelastic scattering of polarised muons on polarised protons and deuterons in the range 0.003 < x < 0.7 and Q2 > 1 GeV2. Compared to our previous publication on this subject, with the new data the statistical errors have been reduced by nearly a factor of two. From these asymmetries and our inclusive spin asymmetries we determine the polarised quark distributions of valence quarks and non-strange sea quarks at Q2 = 10 GeV2. The polarised u valence quark distribution, Δuυ(×), is positive and the polarisation increases with x. The polarised d valence quark distribution, Δdυ(x), is negative and the non-strange sea distribution, Δq-(x), is consistent with zero over the measured range of x. We find for the first moments (latin small letter esh)10Δuυ(x)d x = 0.77 ± 0.10 ± 0.08, (latin small letter esh)10Δdυ(x)d x = -0.52 ± 0.14 ± 0.09 and (latin small letter esh)10Δq-(x)d x = 0.01 ± 0.04 ± 0.03, where we assumed Δu-(x) = Δd-(x). We also determine for the first time the second moments of the valence distributions (latin small letter esh)10xΔqυ(x)d x.

Original languageEnglish
Pages (from-to)180-190
Number of pages11
JournalPhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
Volume420
Issue number1-2
DOIs
Publication statusPublished - 19 Feb 1998

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