Beam spin asymmetry benchmark in the spinless meson electroproduction off the scalar target

C. Ji, H. Choi, A. Lundeen, B. Bakker
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引用次数: 0

Abstract

We discuss the electroproduction of a spinless meson, i.e. pseudoscalar ($0^{-+}$) or scalar ($0^{++}$) meson, off the scalar target. The most general formulation of the differential cross section for the $0^{-+}$ or $0^{++}$ meson process involves only one or two hadronic form factors, respectively, on a scalar target. The Rosenbluth-type separation of the differential cross section provides the explicit relation between the hadronic form factors and the different parts of the differential cross section in a completely model-independent manner. The absence of the beam spin asymmetry for the pseudoscalar meson production provides a benchmark for the experimental data analysis. The measurement of the beam spin asymmetry for the scalar meson production may also provide a unique opportunity not only to explore the imaginary part of the hadronic amplitude in the general formulation but also to examine the significance of the chiral-odd generalized parton distribution (GPD) contribution in the leading-twist GPD formulation.
光束自旋不对称的基准在无自旋介子的电产生上偏离标量目标
我们讨论了无自旋介子的电生产,即假标量介子($0^{-+}$)或标量介子($0^{++}$)介子,远离标量目标。对于$0^{-+}$或$0^{++}$介子过程的微分截面,最一般的公式分别只涉及标量目标上的一个或两个强子形式因子。微分截面的rosenbluth型分离以完全独立于模型的方式提供了强子形状因子与微分截面不同部分之间的明确关系。赝标量介子产生过程中束自旋不对称性的存在为实验数据分析提供了一个基准。对于标量介子产生的束自旋不对称性的测量也提供了一个独特的机会,不仅可以探索一般公式中强子振幅的虚部,而且可以检查手性奇广义部分分布(GPD)在导扭GPD公式中的贡献的意义。
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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