4.4 Article

Nucleon momentum fraction, helicity and transversity from 2+1-flavor lattice QCD

期刊

JOURNAL OF HIGH ENERGY PHYSICS
卷 -, 期 4, 页码 -

出版社

SPRINGER
DOI: 10.1007/JHEP04(2021)044

关键词

Lattice QCD; Lattice Quantum Field Theory

资金

  1. Office of Science of the U.S. Department of Energy [DE-AC02-05CH11231]
  2. DOE Office of Science User Facility [DE-AC05-00OR22725]
  3. INCITE Program project [PHY138]
  4. ALCC program project [LGT107]
  5. Office of Science of the U.S. Department of Energy
  6. U.S. Department of Energy, Office of Science, Office of High Energy Physics [DE-AC52-06NA25396]
  7. U.S. Department of Energy, Office of Science, Office of Nuclear Physics [DE-AC05-06OR23177]
  8. U.S. Department of Energy, Office of Science [DE-AC05-06OR22725]
  9. U.S. Department of Energy, Office of Science, Office of Advanced Scientific Computing Research
  10. Office of Nuclear Physics, Scientific Discovery through Advanced Computing (SciDAC) program
  11. U.S. Department of Energy Exascale Computing Project
  12. LANL LDRD program
  13. Center for Nonlinear Studies

向作者/读者索取更多资源

By analyzing high-statistics data, better control over the systematic uncertainties in the calculation of the isovector momentum fraction, helicity moment, and transversity moment of the nucleon is achieved. The results for these moments are consistent with global fit values.
A detailed analysis of the systematic uncertainties in the calculation of the isovector momentum fraction, < x >(u-d), helicity moment, < x >(Delta u-Delta d), and the transversity moment, < x >(delta u-delta d), of the nucleon is presented using high-statistics data on seven ensembles of gauge configurations generated by the JLab/W&M/LANL/MIT collaborations using 2 + 1-flavors of dynamical Wilson-clover quarks. The much higher statistics have facilitated better control over all systematics compared to previous lattice calculations. The least understood systematic - excited-state contamination - is quantified by studying the variation of the results as a function of different estimates of the mass gap of the first excited state, obtained from two- and three-point correlation functions, and as a function of the pion mass M. The final results are obtained using a simultaneous fit in the lattice spacing a, pion mass M-pi and the finite volume parameter M pi L keeping leading order corrections. The data show no significant dependence on the lattice spacing and some evidence for finite-volume corrections. Our final results, in the (MS) over bar scheme at 2 GeV, are < x >(u-d) = 0.155(17)(20), < x >(Delta u-Delta d) = 0.183(14)(20) and < x >(delta u-delta d) = 0.220(18)(20), where the first error is the overall analysis uncertainty assuming excited-state contributions have been removed, and the second is an additional systematic uncertainty due to possible residual excited-state contributions. These results are consistent with phenomenological global fit values.

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