The MSR mass and the O(Λ[subscript QCD]) renormalon sum rule

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 RenormalonsUnited States. Department of Energy (Grant DE-SC0011090)Simons Foundation (Grant 327942