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arXiv 0802.0863hep-lat
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具有两种动力学畴壁费米子的核子结构

Nucleon structure with two flavors of dynamical domain-wall fermions

Huey-Wen Lin, Tom Blum, Shigemi Ohta, Shoichi Sasaki, Takeshi Yamazaki

摘要:

本文用格子量子色动力学方法计算了核子的等矢量形状因子和等矢量结构函数的前几阶矩。计算采用了两种简并动力学口味的畴壁费米子,从而很好地控制手征对称性破缺。在必要的情况下,进行相关夸克流的非微扰重整化。逆晶格间距$a^{-1}$约为1.7 GeV。我们使用简并的上、下动力学夸克质量分别为奇异夸克质量的1、3/4和1/2。晶格的物理体积约为$(1.9{fm})^3$。随着夸克质量向物理点减小,等矢量与轴向电荷之比$g_A/g_V$趋于略低于实验值。我们计算了动量转移依赖的等矢量矢量,轴向,诱导张量和诱导赝标量形状因子。Goldberger-Treiman关系在低动量转移下成立,并产生一个π-核子耦合,$g_{πNN} = 15.5(1.4)$,其中引用的误差只是统计的。通过线性手征外推,我们发现味夸克非单重态动量分数$<x>_{u-d}$和夸克螺旋度分数$<x>_{Δu-Δd}$超过了实验值。我们得到的横向度,$<1 >_{δu-δd} = 0.93(6)$在$\bar{\rm MS}$在2 GeV和扭转3极化力矩,$d_1$,出现小,这表明Wandzura-Wilczek关系保持近似。我们讨论了计算中的系统误差,特别注意有限体积效应,激发态污染,和手征外推。

英文摘要:

We present a numerical lattice quantum chromodynamics calculation of isovector form factors and the first few moments of the isovector structure functions of the nucleon. The calculation employs two degenerate dynamical flavors of domain-wall fermions, resulting in good control of chiral symmetry breaking. Non-perturbative renormalization of the relevant quark currents is performed where necessary. The inverse lattice spacing, $a^{-1}$, is about 1.7 GeV. We use degenerate up and down dynamical quark masses around 1, 3/4 and 1/2 the strange quark mass. The physical volume of the lattice is about $(1.9{fm})^3$. The ratio of the isovector vector to axial charges, $g_A/g_V$, trends a bit lower than the experimental value as the quark mass is reduced toward the physical point. We calculate the momentum-transfer dependences of the isovector vector, axial, induced tensor and induced pseudoscalar form factors. The Goldberger-Treiman relation holds at low momentum transfer and yields a pion-nucleon coupling, $g_{πNN} = 15.5(1.4)$, where the quoted error is only statistical. We find that the flavor non-singlet quark momentum fraction $<x>_{u-d}$ and quark helicity fraction $<x>_{Δu-Δd}$ overshoot their experimental values after linear chiral extrapolation. We obtain the transversity, $<1 >_{δu-δd} = 0.93(6)$ in $\bar{\rm MS}$ at 2 GeV and a twist-3 polarized moment, $d_1$, appears small, suggesting that the Wandzura-Wilczek relation holds approximately. We discuss the systematic errors in the calculation, with particular attention paid to finite-volume effects, excited-state contamination, and chiral extrapolations.

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