格子 QCD 中的奇极性核子电磁跃迁

Finn M. Stokes, Benjamin J. Owen, Waseem Kamleh, Derek B. Leinweber
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引用次数: 0

摘要

奇偶性扩展变分分析(PEVA)技术能够分离出有限动量下的反奇偶性特征状态。这种方法已被用于对激发重子形式因子进行首次格子 QCD 计算。特别是,这些计算表明,在中等u夸克和d夸克质量接近奇异夸克质量时,低洼奇偶核子激发可以用组成夸克模型很好地描述。在这里,我们扩展了PEVA技术,建立了一个确定格子QCD中奇副核电磁转变形式因子的形式主义。我们首次计算了从基态核子到前两个奇偶性激发的转换的螺旋振幅。通过与组成夸克模型对这些振幅的计算结果进行比较,这些新结果给出了对这些激发结构的重要见解。这项工作是将$N^*(1535)$和$N^*(1650)$共振的实验电导振幅与非原位格子QCD计算相比较的关键一步。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Odd-Parity Nucleon Electromagnetic Transitions in Lattice QCD
The parity-expanded variational analysis (PEVA) technique enables the isolation of opposite-parity eigenstates at finite momentum. The approach has been used to perform the first lattice QCD calculations of excited-baryon form factors. In particular, these calculations show that the low-lying odd-parity nucleon excitations are described well by constituent quark models at moderate u and d quark masses approaching the strange quark mass. Herein, we extend the PEVA technique to establish a formalism for the determination of odd-parity nucleon electromagnetic transition form factors in lattice QCD. The formalism is implemented in the first calculation of the helicity amplitudes for transitions from the ground state nucleon to the first two odd-parity excitations. Through a comparison with constituent quark model calculations of these amplitudes, these new results give important insight into the structure of these excitations. This work is a critical step towards confronting experimental electroproduction amplitudes for the $N^*(1535)$ and $N^*(1650)$ resonances with ab-initio lattice QCD calculations.
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