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Measurement of the proton spin structure at long distances

  • X. Zheng
  • , A. Deur
  • , H. Kang
  • , S. E. Kuhn
  • , M. Ripani
  • , J. Zhang
  • , K. P. Adhikari
  • , S. Adhikari
  • , M. J. Amaryan
  • , H. Atac
  • , H. Avakian
  • , L. Barion
  • , M. Battaglieri
  • , I. Bedlinskiy
  • , F. Benmokhtar
  • , A. Bianconi
  • , A. S. Biselli
  • , S. Boiarinov
  • , M. Bondì
  • , F. Bossù
  • P. Bosted, W. J. Briscoe, J. Brock, W. K. Brooks, D. Bulumulla, V. D. Burkert, C. Carlin, D. S. Carman, J. C. Carvajal, A. Celentano, P. Chatagnon, T. Chetry, J. P. Chen, S. Choi, G. Ciullo, L. Clark, P. L. Cole, M. Contalbrigo, V. Crede, A. D’Angelo, N. Dashyan, R. De Vita, M. Defurne, S. Diehl, C. Djalali, V. A. Drozdov, R. Dupre, M. Ehrhart, A. El Alaoui, L. El Fassi, L. Elouadrhiri, P. Eugenio, G. Fedotov, S. Fegan, R. Fersch, A. Filippi, T. A. Forest, Y. Ghandilyan, G. P. Gilfoyle, K. L. Giovanetti, F. X. Girod, D. I. Glazier, R. W. Gothe, K. A. Griffioen, M. Guidal, N. Guler, L. Guo, K. Hafidi, H. Hakobyan, M. Hattawy, T. B. Hayward, D. Heddle, K. Hicks, A. Hobart, T. Holmstrom, M. Holtrop, Y. Ilieva, D. G. Ireland, E. L. Isupov, H. S. Jo, K. Joo, S. Joosten, C. D. Keith, D. Keller, A. Khanal, M. Khandaker, C. W. Kim, W. Kim, F. J. Klein, A. Kripko, V. Kubarovsky, L. Lanza, M. Leali, P. Lenisa, K. livingston, E. Long, I. J.D. MacGregor, N. Markov, L. Marsicano, V. Mascagna, B. McKinnon, D. G. Meekins, T. Mineeva, M. Mirazita, V. Mokeev, C. Mullen, P. Nadel-Turonski, K. Neupane, S. Niccolai, M. Osipenko, A. I. Ostrovidov, M. Paolone, L. Pappalardo, K. Park, E. Pasyuk, W. Phelps, S. K. Phillips, O. Pogorelko, J. Poudel, Y. Prok, B. A. Raue, J. Ritman, A. Rizzo, G. Rosner, P. Rossi, J. Rowley, F. Sabatié, C. Salgado, A. Schmidt, R. A. Schumacher, M. L. Seely, Y. G. Sharabian, U. Shrestha, S. Širca, K. Slifer, N. Sparveris, S. Stepanyan, I. I. Strakovsky, S. Strauch, V. Sulkosky, N. Tyler, M. Ungaro, L. Venturelli, H. Voskanyan, E. Voutier, D. P. Watts, X. Wei, L. B. Weinstein, M. H. Wood, B. Yale, N. Zachariou, Z. W. Zhao
  • University of Virginia
  • Thomas Jefferson National Accelerator Facility
  • Seoul National University
  • Old Dominion University
  • National Institute for Nuclear Physics
  • Mississippi State University
  • Hampton University
  • Florida International University
  • Temple University
  • Russian Research Centre Kurchatov Institute
  • Duquesne University
  • University of Brescia
  • Fairfield University
  • Université Paris-Saclay
  • College of William and Mary
  • George Washington University
  • Universidad Técnica Federico Santa Maria
  • University of Ferrara
  • University of Glasgow
  • Lamar University
  • Idaho State University
  • Florida State University
  • University of Rome Tor Vergata
  • A. Alikhanian Yerevan Institute of Physics
  • Justus Liebig University Giessen
  • University of Connecticut
  • Ohio University
  • University of South Carolina
  • Lomonosov Moscow State University
  • Argonne National Laboratory
  • University of York
  • Christopher Newport University
  • University of Richmond
  • James Madison University
  • University of New Hampshire
  • Norfolk State University
  • Kyungpook National University
  • Catholic University of America
  • Rensselaer Polytechnic Institute
  • University of Insubria
  • Jülich Research Centre
  • Carnegie Mellon University
  • University of Ljubljana
  • Canisius College

Research output: Contribution to journalArticlepeer-review

30 Scopus citations

Abstract

Measuring the spin structure of protons and neutrons tests our understanding of how they arise from quarks and gluons, the fundamental building blocks of nuclear matter. At long distances, the coupling constant of the strong interaction becomes large, requiring non-perturbative methods to calculate quantum chromodynamics processes, such as lattice gauge theory or effective field theories. Here we report proton spin structure measurements from scattering a polarized electron beam off polarized protons. The spin-dependent cross-sections were measured at large distances, corresponding to the region of low momentum transfer squared between 0.012 and 1.0 GeV2. This kinematic range provides unique tests of chiral effective field theory predictions. Our results show that a complete description of the nucleon spin remains elusive, and call for further theoretical works, for example, in lattice quantum chromodynamics. Finally, our data extrapolated to the photon point agree with the Gerasimov–Drell–Hearn sum rule, a fundamental prediction of quantum field theory that relates the anomalous magnetic moment of the proton to its integrated spin-dependent cross-sections.

Original languageEnglish
Pages (from-to)736-741
Number of pages6
JournalNature Physics
Volume17
Issue number6
DOIs
StatePublished - Jun 2021

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