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晶格量子色动力学中量子色动力学耦合精度测定的过去、现在与未来。

Past, present, and future of precision determinations of the QCD coupling from lattice QCD.

作者信息

Dalla Brida Mattia

机构信息

Dipartimento di Fisica, Università di Milano-Bicocca, Piazza della Scienza 3, 20126 Milan, Italy.

INFN, Sezione di Milano-Bicocca, Piazza della Scienza 3, 20126 Milan, Italy.

出版信息

Eur Phys J A Hadron Nucl. 2021;57(2):66. doi: 10.1140/epja/s10050-021-00381-3. Epub 2021 Feb 22.

DOI:10.1140/epja/s10050-021-00381-3
PMID:33642940
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7898597/
Abstract

Non-perturbative scale-dependent renormalization problems are ubiquitous in lattice QCD as they enter many relevant phenomenological applications. They require solving non-perturbatively the renormalization group equations for the QCD parameters and matrix elements of interest in order to relate their non-perturbative determinations at low energy to their high-energy counterparts needed for phenomenology. Bridging the large energy separation between the hadronic and perturbative regimes of QCD, however, is a notoriously difficult task. In this contribution we focus on the case of the QCD coupling. We critically address the common challenges that state-of-the-art lattice determinations have to face in order to be significantly improved. In addition, we review a novel strategy that has been recently put forward in order to solve this non-perturbative renormalization problem and discuss its implications for future precision determinations. The new ideas exploit the decoupling of heavy quarks to match -flavor QCD and the pure Yang-Mills theory. Through this matching the computation of the non-perturbative running of the coupling in QCD can be shifted to the computationally much easier to solve pure-gauge theory. We shall present results for the determination of the -parameter of -flavor QCD where this strategy has been applied and proven successful. The results demonstrate that these techniques have the potential to unlock unprecedented precision determinations of the QCD coupling from the lattice. The ideas are moreover quite general and can be considered to solve other non-perturbative renormalization problems.

摘要

非微扰标度依赖的重整化问题在格点量子色动力学(lattice QCD)中无处不在,因为它们出现在许多相关的唯象学应用中。为了将低能下的非微扰确定值与唯象学所需的高能对应值联系起来,需要非微扰地求解量子色动力学参数和感兴趣的矩阵元的重整化群方程。然而,弥合量子色动力学强子 regime 和微扰 regime 之间的巨大能量间隔是一项极其困难的任务。在本论文中,我们聚焦于量子色动力学耦合常数的情况。我们批判性地探讨了最先进的格点确定值为了得到显著改进所必须面对的常见挑战。此外,我们回顾了最近提出的一种新颖策略,以解决这个非微扰重整化问题,并讨论其对未来高精度确定值的影响。新的思路利用重夸克的解耦来匹配(n_f)味量子色动力学和纯杨 - 米尔斯理论。通过这种匹配,量子色动力学中耦合常数的非微扰跑动计算可以转移到计算上更容易求解的纯规范理论中。我们将展示在应用并证明该策略成功的(n_f)味量子色动力学(\beta)参数确定方面的结果。结果表明,这些技术有潜力从格点获得前所未有的高精度量子色动力学耦合常数确定值。而且这些思路相当通用,可以被认为用于解决其他非微扰重整化问题。

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