Unpolarized gluon distribution in the nucleon from lattice quantum chromodynamics

被引:28
作者
Khan, Tanjib [1 ]
Sufian, Raza Sabbir [1 ,2 ]
Karpie, Joseph [3 ]
Monahan, Christopher J. [1 ,2 ]
Egerer, Colin [1 ,2 ]
Joo, Balint [4 ]
Morris, Wayne [2 ,5 ]
Orginos, Kostas [1 ,2 ]
Radyushkin, Anatoly [2 ,5 ]
Richards, David G. [2 ]
Romero, Eloy [2 ]
Zafeiropoulos, Savvas [6 ]
机构
[1] William & Mary, Dept Phys, Williamsburg, VA 23185 USA
[2] Thomas Jefferson Natl Accelerator Facil, Newport News, VA 23606 USA
[3] Columbia Univ, Dept Phys, New York, NY 10027 USA
[4] Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA
[5] Old Dominion Univ, Dept Phys, Norfolk, VA 23529 USA
[6] Aix Marseille Univ, Univ Toulon, CPT, CNRS, Marseille, France
基金
美国国家科学基金会;
关键词
SCATTERING; MATRIX;
D O I
10.1103/PhysRevD.104.094516
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
In this study, we present a determination of the unpolarized gluon Ioffe-time distribution in the nucleon from a first principles lattice quantum chromodynamics calculation. We carry out the lattice calculation on a 32(3) x 64 ensemble with a pion mass of 358 MeV and lattice spacing of 0.094 fm. We construct the nucleon interpolating fields using the distillation technique, flow the gauge fields using the gradient flow, and solve the summed generalized eigenvalue problem to determine the gluonic matrix elements. Combining these techniques allows us to provide a statistically well-controlled Ioffe-time distribution and unpolarized gluon parton distribution function. We obtain the flow time independent reduced Ioffe-time pseudodistribution and calculate the light-cone Ioffe-time distribution and unpolarized gluon distribution function in the (MS) over bar scheme at mu = 2 GeV, neglecting the mixing of the gluon operator with the quark singlet sector. Finally, we compare our results to phenomenological determinations.
引用
收藏
页数:19
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