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

被引:2
作者
Mondal, Santanu [1 ]
Gupta, Rajan [1 ]
Park, Sungwoo [1 ,2 ]
Yoon, Boram [3 ]
Bhattacharya, Tanmoy [1 ]
Joo, Balint [4 ]
Winter, Frank [5 ]
机构
[1] Los Alamos Natl Lab, Theoret Div T2, Los Alamos, NM 87545 USA
[2] Los Alamos Natl Lab, Ctr Nonlinear Studies, Los Alamos, NM 87545 USA
[3] Los Alamos Natl Lab, Comp Computat & Stat Sci, CCS 7, Los Alamos, NM 87545 USA
[4] Oak Ridge Natl Lab, Oak Ridge Leadership Comp Facil, POB 2009, Oak Ridge, TN 37831 USA
[5] Jefferson Lab, 12000 Jefferson Ave, Newport News, VA 23606 USA
关键词
Lattice QCD; Lattice Quantum Field Theory; BARYON OCTET;
D O I
10.1007/JHEP04(2021)044
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
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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页数:37
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