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arXiv 2201.08367hep-lat
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康普顿振幅、格点量子色动力学和Feynman-Hellmann方法

The Compton Amplitude, lattice QCD and the Feynman-Hellmann approach

K. U. Can, A. Hannaford-Gunn, R. Horsley, Y. Nakamura, H. Perlt, P. E. L. Rakow, E. Sankey, G. Schierholz, H. Stüben, R. D. Young, J. M. Zanotti

摘要:

格点量子色动力学的一个主要目标是计算强子矩阵元。标准方法是使用三点和四点关联函数。另一种方法,只需要计算两点关联函数是使用费曼-赫尔曼定理。在这次演讲中,我们将这种方法发展到二阶微扰理论,在适当的格点量子色动力学的背景下。这包括康普顿振幅(形成深度非弹性散射的基础)和强子散射。一些数值结果表明这种方法可能实现的结果。

英文摘要:

A major objective of lattice QCD is the computation of hadronic matrix elements. The standard method is to use three-point and four-point correlation functions. An alternative approach, requiring only the computation of two-point correlation functions is to use the Feynman-Hellmann theorem. In this talk we develop this method up to second order in perturbation theory, in a context appropriate for lattice QCD. This encompasses the Compton Amplitude (which forms the basis for deep inelastic scattering) and hadron scattering. Some numerical results are presented showing results indicating what this approach might achieve.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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