Beam Spin Asymmetries of \(\pi ^{ + }\pi ^{0}\) Dihadrons from SIDIS at CLAS12

C. Dilks
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Abstract

Spin asymmetries provide a wide range of insights into nucleon structure and hadronization. Recent measurements of beam spin asymmetries of π + π − dihadrons from Semi-Inclusive Deep Inelastic Scattering (SIDIS) at CLAS12 provide the first empirical evidence of a nonzero G ⊥ 1 , the parton helicity-dependent Dihadron Fragmentation Function (DiFF) encoding spin-momentum correlations in hadronization. These measurements have been extended to aid in the characterization of H ⊥ 1 and H ∢ 1 , the DiFFs dependent on parton transverse spin, via a multidimensional partial wave analysis, giving access to the dependence on the interference of dihadrons of particular polarizations. Reconstruction of π 0 s allows for further extension of these measurements to π + π 0 and π − π 0 dihadrons. The DiFFs describing π + π − production differ from those describing π + π 0 and π − π 0 production, which involve different quark flavors along with a strong suppression of the exclusive diffractive contribution. This presentation will focus on beam spin asymmetries for π + π 0 dihadrons, compared to those from π + π − dihadrons, which will help shed light on a more comprehensive picture of dihadron fragmentation.
来自SIDIS的\(\pi ^{ + }\pi ^{0}\)双强子束自旋不对称性
自旋不对称为核子结构和强子化提供了广泛的见解。最近在CLAS12的半包容深度非弹性散射(SIDIS)中对π + π−对偶强子束自旋不对称性的测量提供了非零g⊥的第一个经验证据,这是一种与部分螺旋度相关的对偶强子碎片函数(DiFF),编码强子化中的自旋动量相关。这些测量已被扩展,以通过多维部分波分析来帮助表征H⊥和H⊥,即依赖于部分子横向自旋的DiFFs,从而获得对特定极化的对强子干涉的依赖。π 0 s的重建允许将这些测量进一步扩展到π + π 0和π−π 0对强子。描述π + π−产生的DiFFs不同于描述π + π 0和π−π 0产生的DiFFs,它们涉及不同的夸克口味以及对专属衍射贡献的强烈抑制。本演讲将重点讨论π + π 0对强子的光束自旋不对称性,与π + π−对强子的光束自旋不对称性进行比较,这将有助于阐明对强子分裂的更全面的图景。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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