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格点量子色动力学对μ子反常磁矩的强子光致光散射贡献。

Hadronic light-by-light scattering contribution to the muon anomalous magnetic moment from lattice QCD.

作者信息

Blum Thomas, Chowdhury Saumitra, Hayakawa Masashi, Izubuchi Taku

机构信息

Physics Department, University of Connecticut, Storrs, Connecticut 06269-3046, USA and RIKEN BNL Research Center, Brookhaven National Laboratory, Upton, New York 11973, USA.

Physics Department, University of Connecticut, Storrs, Connecticut 06269-3046, USA.

出版信息

Phys Rev Lett. 2015 Jan 9;114(1):012001. doi: 10.1103/PhysRevLett.114.012001. Epub 2015 Jan 7.

DOI:10.1103/PhysRevLett.114.012001
PMID:25615460
Abstract

The most compelling possibility for a new law of nature beyond the four fundamental forces comprising the standard model of high-energy physics is the discrepancy between measurements and calculations of the muon anomalous magnetic moment. Until now a key part of the calculation, the hadronic light-by-light contribution, has only been accessible from models of QCD, the quantum description of the strong force, whose accuracy at the required level may be questioned. A first principles calculation with systematically improvable errors is needed, along with the upcoming experiments, to decisively settle the matter. For the first time, the form factor that yields the light-by-light scattering contribution to the muon anomalous magnetic moment is computed in such a framework, lattice QCD+QED and QED. A nonperturbative treatment of QED is used and checked against perturbation theory. The hadronic contribution is calculated for unphysical quark and muon masses, and only the diagram with a single quark loop is computed for which statistically significant signals are obtained. Initial results are promising, and the prospect for a complete calculation with physical masses and controlled errors is discussed.

摘要

在构成高能物理标准模型的四种基本力之外,自然界新定律最令人信服的可能性在于μ子反常磁矩的测量值与计算值之间的差异。到目前为止,计算中的一个关键部分,即强子真空极化贡献,只能从量子色动力学(QCD,强力的量子描述)的模型中获得,而该模型在所需精度水平上的准确性可能受到质疑。需要进行具有系统可改进误差的第一性原理计算,并结合即将开展的实验,以果断解决这个问题。首次在这样的框架,即晶格QCD+QED和QED中,计算了产生μ子反常磁矩的轻子-轻子散射贡献的形状因子。采用了量子电动力学(QED)的非微扰处理方法,并与微扰理论进行了对比检验。针对非物理夸克和μ子质量计算了强子贡献,并且仅计算了获得具有统计显著性信号的单夸克圈图。初步结果很有希望,并且讨论了使用物理质量和可控误差进行完整计算的前景。

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引用本文的文献

1
The anomalous magnetic moment of the muon: status of lattice QCD calculations.μ子的反常磁矩:晶格量子色动力学计算的现状
Eur Phys J A Hadron Nucl. 2021;57(4):116. doi: 10.1140/epja/s10050-021-00426-7. Epub 2021 Apr 6.
2
Effects of longitudinal short-distance constraints on the hadronic light-by-light contribution to the muon .纵向短距离约束对强子光致轻子对μ子贡献的影响
Eur Phys J C Part Fields. 2020;80(12):1108. doi: 10.1140/epjc/s10052-020-08611-6. Epub 2020 Dec 2.
3
Dispersive analysis of the pion transition form factor.
π介子跃迁形状因子的色散分析。
Eur Phys J C Part Fields. 2014;74(11):3180. doi: 10.1140/epjc/s10052-014-3180-0. Epub 2014 Nov 27.