4.7 Article

Complete flavor decomposition of the spin and momentum fraction of the proton using lattice QCD simulations at physical pion mass

期刊

PHYSICAL REVIEW D
卷 101, 期 9, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.101.094513

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资金

  1. U.S. Department of Energy, Office of Nuclear Physics
  2. DOE Early Career Award [DE-SC0020405]
  3. Cyprus Research Promotion foundation [POST-DOC/0718/0100, COMPLEMENTARY/0916/0015]
  4. project Nucleon parton distribution functions using Lattice Quantum Chromodynamics - University of Cyprus
  5. project Quantum Fields on the lattice - University of Cyprus
  6. Horizon 2020 research and innovation program of the European Commission under the Marie Sklodowska-Curie Grant [642069]
  7. Gauss Centre for Supercomputing e.V. [pr74yo]
  8. Centro Svizzero di Calcolo Scientifico (CSCS) [s702]
  9. National Science Foundation [TG-PHY170022, 1625061]
  10. U.S. Army Research Laboratory [W911NF-16-2-0189]
  11. John von Neumann-Institute for Computing on the Jureca system at the research center in Julich [ECY00]
  12. U.S. Department of Energy (DOE) [DE-SC0020405] Funding Source: U.S. Department of Energy (DOE)

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We evaluate the gluon and quark contributions to the spin of the proton using an ensemble of gauge configurations generated at physical pion mass. We compute all valence and sea quark contributions to high accuracy. We perform a nonperturbative renormalization for both quark and gluon matrix elements. We find that the contribution of the up, down, strange, and charm quarks to the proton intrinsic spin is 1/2 Sigma(q=u,d,s,c) Delta Sigma(q+) = 0.191(15) and to the total spin Sigma(q=u,d,s,c) Jq(+) = 0.285(45)(10). The gluon contribution to the spin is J(g) = 0.187(46)(10) yielding J = J(q) + J(g) = 0.473(71)(14) confirming the spin sum. The momentum fraction carried by quarks in the proton is found to be 0.618(60) and by gluons 0.427(92), the sum of which gives 1.045(118) confirming the momentum sum rule. All scale and scheme dependent quantities are given in the (MS) over bar scheme at 2 GeV.

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