The MSR mass and the O(Λ[subscript QCD]) renormalon sum rule
Author(s)
Hoang, André H; Jain, Ambar; Lepenik, Christopher; Mateu, Vicent; Scimemi, Ignazio; Stewart, Iain W; Hoang, André H.; Preisser, Moritz; ... Show more Show less
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We provide a detailed description and analysis of a low-scale short-distance mass scheme, called the MSR mass, that is useful for high-precision top quark mass determinations, but can be applied for any heavy quark Q. In contrast to earlier low-scale short-distance mass schemes, the MSR scheme has a direct connection to the well known [bar over MS] mass commonly used for high-energy applications, and is determined by heavy quark on-shell self-energy Feynman diagrams. Indeed, the MSR mass scheme can be viewed as the simplest extension of the [bar over MS] mass concept to renormalization scales ≪ m[subscript Q]. The MSR mass depends on a scale R that can be chosen freely, and its renormalization group evolution has a linear dependence on R, which is known as R-evolution. Using R-evolution for the MSR mass we provide details of the derivation of an analytic expression for the normalization of the O(Λ[subscript QCD]) renormalon asymptotic behavior of the pole mass in perturbation theory. This is referred to as the O(Λ[subscript QCD]) renormalon sum rule, and can be applied to any perturbative series. The relations of the MSR mass scheme to other low-scale short-distance masses are analyzed as well. Keywords: Heavy Quark Physics, Perturbative QCD, Quark Masses and SM Parameters, Renormalization Regularization and Renormalons
Date issued
2018-04Department
Massachusetts Institute of Technology. Center for Theoretical Physics; Massachusetts Institute of Technology. Department of PhysicsJournal
Journal of High Energy Physics
Publisher
Springer Berlin Heidelberg
Citation
Hoang, André H., et al. “The MSR Mass and the O (Λ[subscript QCD] Renormalon Sum Rule.” Journal of High Energy Physics, vol. 2018, no. 4, Apr. 2018. © 2017 Springer International Publishing AG
Version: Final published version
ISSN
1029-8479