Pole mass renormalon and its ramifications
arXiv:2108.04861 · doi:10.1140/epjs/s11734-021-00268-w
Abstract
I review the structure of the leading infrared renormalon divergence of the relation between the pole mass and the mass of a heavy quark, with applications to the top, bottom and charm quark. That the pole quark mass definition must be abandoned in precision computations is a well-known consequence of the rapidly diverging series. The definitions and physics motivations of several leading renormalon-free, short-distance mass definitions suitable for processes involving nearly on-shell heavy quarks are discussed.
23 pages, LaTex, contribution to EPJ ST "Renormalons and Hyperasymptotics in QCD"; v2: missing minus signs in tables 2 and 3 corrected
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- Reconciling the Contour-Improved and Fixed-Order Approaches for Hadronic Spectral Moments II: Renormalon Norm and Application in Determinations
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- The width difference in the system at next-to-next-to-leading order of QCD
- Testing parton distribution functions with t-channel single-top-quark production
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- Revisiting lifetimes of doubly charmed baryons
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- On-shell Matrix Elements of the EMT Trace in Gauge Theories and Heavy Quark Masses
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- Measurement of the top-quark pole mass in dileptonic events at TeV with the ATLAS experiment
- Reconciling the FOPT and CIPT Predictions for the Hadronic Tau Decay Rate
- ILM gluons in perturbative QCD