论文标题

核子动量分数,螺旋性和从2+1味晶格QCD的横向性

Nucleon Momentum Fraction, Helicity and Transversity from 2+1-flavor Lattice QCD

论文作者

Mondal, Santanu, Gupta, Rajan, Park, Sungwoo, Yoon, Boram, Bhattacharya, Tanmoy, Joó, Bálint, Winter, Frank

论文摘要

ISOVECTOR动量分数的高统计结果,$ \ langle x \ rangle_ {u-d} $,螺旋力矩,$ \ langle x \ rangle_ {ΔU-Δd} $,terranstersity artversity artment,$ \ langle x \ langle x \ rangle_ {通过JLAB/W&M/LANL/MIT合作,使用$ 2+1 $ - 动态的Wilson-Clover Quarks。注意理解和控制激发态的贡献。最终结果是使用晶格间距$ a $,pion $m_π$和有限体积参数$m_πl$的同时拟合获得的。数据显示,对晶格间距没有显着依赖,也没有有限体积校正的一些证据。主要变化是$m_π$,其大小取决于分析中使用的第一个激发态的质量间隙。我们的最终结果是在2 Gev的$ \ Overline {\ rm MS} $方案中,是$ \ langle x \ rangle_ {u-d} = 0.160(16)(20)$,$ \ langle x \ rangle_ \ rangle_ {ΔU-ΔD} = 0.215(17)(20)$,其中第一个误差是假设兴奋状态贡献已被删除的总体分析不确定性,第二个误差是由于可能的残留兴奋状态贡献而导致的额外系统不确定性。这些结果与其他最近的晶格计算和现象学全球拟合值一致。

High statistics results for the isovector momentum fraction, $\langle x \rangle_{u-d}$, helicity moment, $\langle x \rangle_{Δu-Δd}$, and the transversity moment, $\langle x\rangle_{δu-δd}$, of the nucleon are presented using seven ensembles of gauge configurations generated by the JLab/W&M/LANL/MIT collaborations using $2+1$-flavors of dynamical Wilson-clover quarks. Attention is given to understanding and controlling the contributions of excited states. The final results are obtained using a simultaneous fit in the lattice spacing $a$, pion mass $M_π$ and the finite volume parameter $M_πL$ keeping leading order corrections. The data show no significant dependence on the lattice spacing and some evidence for finite-volume corrections. The main variation is with $M_π$, whose magnitude depends on the mass gap of the first excited state used in the analysis. Our final results, in the $\overline{\rm MS}$ scheme at 2 GeV, are $\langle x \rangle_{u-d} = 0.160(16)(20)$, $\langle x \rangle_{Δu-Δd} = 0.192(13)(20)$ and $\langle x \rangle_{δu-δd} = 0.215(17)(20)$, 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 other recent lattice calculations and phenomenological global fit values.

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