4.7 Article

Parton distribution functions beyond leading twist from lattice QCD: The hL (x) case

期刊

PHYSICAL REVIEW D
卷 104, 期 11, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.104.114510

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资金

  1. National Science Foundation [PHY-1812359]
  2. U.S. Department of Energy, Office of Science, Office of Nuclear Physics [DE-SC0020405]
  3. National Science Centre (Poland) [2016/22/E/ST2/00013]
  4. NSFC [12070131001]
  5. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) [TRR110, 196253076-TRR 110]
  6. Office of Science of the U.S. Department of Energy
  7. PLGrid Infrastructure (Prometheus supercomputer at AGH Cyfronet in Cracow)

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In this study, the isovector flavor combination of the chiral-odd twist-3 parton distribution h(L) (x) for the proton was calculated rapidly using lattice QCD techniques. The results were renormalized nonperturbatively and presented in the (MS) over bar scheme at the scale of 2 GeV. Additionally, the transversity distribution h(1) (x) was also computed and compared to its Wandzura-Wilczek approximation.
We report the fast-ever calculation of the isovector flavor combination of the chiral-odd twist-3 parton distribution h(L) (x) for the proton from lattice QCD. We employ gauge configurations with two degenerate light, a strange and a charm quark (N-f = 2 + 1 + 1) of maximally twisted mass fermions with a clover improvement. The lattice has a spatial extent of 3 fm and lattice spacing of 0.093 fm. The values of the quark masses lead to a pion mass of 260 MeV. We use a source-sink time separation of 1.12 fm to control contamination from excited states. Our calculation is based on the quasi-distribution approach, with three values for the proton momentum: 0.83, 1.25, and 1.67 GeV. The lattice data are renormalized nonperturbatively using the RI' scheme, and the final result for h(L) (x) is presented in the (MS) over bar scheme at the scale of 2 GeV. Furthermore, we compute in the same setup the transversity distribution, h(1) (x), which allows us, in particular, to compare h(L) (x) to its Wandzura-Wilczek approximation. We also combine results for the isovector and isoscalar flavor combinations to disentangle the individual quark contributions for h(1) (x) and h(L) (x), and address the Wandzura-Wilczek approximation in that case as well.

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