2008/01/07 by A. W. Thomas, Jefferson Lab · 1 citation
Physics and Astronomy · #Anomaly (physics) #Gluon #High-Energy Particle Collisions Research #Muon #Nuclear physics #Nucleon #Particle physics #Particle physics theoretical and experimental studies #Physics #Proton #Proton spin crisis #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Quark #Spin (aerodynamics) #hep-ph
paper · pdf · doi:10.1016/j.ppnp.2007.12.039
published as Prog.Part.Nucl.Phys.61:219-228,2008 · Invited lecture presented at Erice: International School of Nuclear Physics, Course 29, Quarks in Hadrons and Nuclei (September 16-24, 2007)
openalex publication_date 2008/01/07 · arxiv created 2008/05/28 · arxiv updated 2010/11/11 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The twenty years since the announcement of the proton spin crisis by the European Muon Collaboration has seen tremendous progress in our knowledge of the distribution of spin within the proton. The problem is reviewed, beginning with the original data and the suggestion that polarized gluons may play a crucial role in resolving the problem through the U(1) axial anomaly. The discussion continues to the present day where not only have strong limits have been placed on the amount of polarized glue in the proton but the experimental determination of the spin content has become much more precise. It is now clear that the origin of the discrepancy between experiment and the naive expectation of the fraction of spin carried by the quarks and anti-quarks in the proton lies in the non-perturabtive structure of the proton. We explain how the features expected in a modern, relativistic and chirally symmetric description of nucleon structure naturally explain the current data.