The heavy quark pole mass in perturbation theory suffers from a renormalon caused, inherent uncertainty of $O(\Lambda_{\rm QCD})$. This fundamental difficulty of determining the pole mass to an accuracy better than the inherent uncertainty can be overcome by direct resummation of the first infrared renormalon. We show how a properly defined pole mass as well as the $\bar {\rm MS}$ mass for the top and bottom quarks can be determined accurately from the $O(m\alpha_s^5)$ quarkonium ground state energy
We provide a systematic renormalization group formalism for the mass effects in the relation of the ...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
I review the structure of the leading infrared renormalon divergence of the relation between the pol...
We show that the pole mass of a heavy quark cannot be extracted from the quarkonium spectrum with an...
We combine the known asymptotic behaviour of the QCD perturbation series expansion, which relates th...
The effective charges motivated method is applied to the relation between pole and M̅S̅-scheme heavy...
We present the next-to-next-to-next-to-leading O(#alpha#_s"5m_q) result for the ground state en...
We provide a detailed description and analysis of a low-scale short-distance mass scheme, called the...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Abstract We provide a detailed description and analysis of a low-scale short-distance mass scheme, c...
We obtain an improved determination of the normalization constant of the first infrared renormalon o...
The top quark pole mass is affected by perturbative divergences known as renormalons, therefore this...
We present an evaluation of heavy quarkonium states (bottomium and charmonium) from first principles...
We provide a systematic renormalization group formalism for the mass effects in the relation of the ...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
I review the structure of the leading infrared renormalon divergence of the relation between the pol...
We show that the pole mass of a heavy quark cannot be extracted from the quarkonium spectrum with an...
We combine the known asymptotic behaviour of the QCD perturbation series expansion, which relates th...
The effective charges motivated method is applied to the relation between pole and M̅S̅-scheme heavy...
We present the next-to-next-to-next-to-leading O(#alpha#_s"5m_q) result for the ground state en...
We provide a detailed description and analysis of a low-scale short-distance mass scheme, called the...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Abstract We provide a detailed description and analysis of a low-scale short-distance mass scheme, c...
We obtain an improved determination of the normalization constant of the first infrared renormalon o...
The top quark pole mass is affected by perturbative divergences known as renormalons, therefore this...
We present an evaluation of heavy quarkonium states (bottomium and charmonium) from first principles...
We provide a systematic renormalization group formalism for the mass effects in the relation of the ...
Precision determinations of the top-quark mass require theory predictions with a well-defined mass p...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...