We update determination of the MS‾ masses of the charm and bottom quarks, from comparisons of the masses of the charmonium and bottomonium 1S states with their perturbative predictions up to next-to-next-to-next-to-leading order in ε expansion and using the MS‾ masses. Effects of non-zero charm-quark mass in the bottomonium masses are incorporated up to next-to-next-to-leading order. We obtain m‾c=1246±2(d3)±4(αs)±23(h.o.) MeV and m‾b=4197±2(d3)±6(αs)±20(h.o.)±5(mc) MeV, which agree with the current Particle Data Group values
In this paper we compare recent experimental data for the total cross section σ ( e + e − →hadrons) ...
We determine the MS-bar charm quark mass from a charmonium QCD sum rules analysis. On the theoretica...
We provide a new determination of the charm quark mass using the Highly Improved Staggered Quark (HI...
AbstractWe update determination of the MS‾ masses of the charm and bottom quarks, from comparisons o...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
Abstract The bottomonium spectrum up to n = 3 is studied within Non-Relativistic Quantum Chromodynam...
The first value is the “running mass ” mb(µ = mb) in the MS scheme, and the second value is the 1S m...
Using a new result for the first moment of the hadronic production cross section at order ${\cal O}(...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
We obtain an improved determination of the normalization constant of the first infrared renormalon o...
Recent theoretical and experimental improvements in the determination of charm and bottom quark mass...
We update the experimental moments for the charm quark as computed in [J. H. Kühn, M. Steinhauser, a...
We update the experimental moments for the charm quark as computed in arXiv:hep-ph/0702103. and used...
In this talk we discuss results of a new extraction of the MS charm quark mass using relativistic QC...
The first value is the “running mass ” mb(µ = mb) in the MS scheme, and the second value is the 1S m...
In this paper we compare recent experimental data for the total cross section σ ( e + e − →hadrons) ...
We determine the MS-bar charm quark mass from a charmonium QCD sum rules analysis. On the theoretica...
We provide a new determination of the charm quark mass using the Highly Improved Staggered Quark (HI...
AbstractWe update determination of the MS‾ masses of the charm and bottom quarks, from comparisons o...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
Abstract The bottomonium spectrum up to n = 3 is studied within Non-Relativistic Quantum Chromodynam...
The first value is the “running mass ” mb(µ = mb) in the MS scheme, and the second value is the 1S m...
Using a new result for the first moment of the hadronic production cross section at order ${\cal O}(...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
We obtain an improved determination of the normalization constant of the first infrared renormalon o...
Recent theoretical and experimental improvements in the determination of charm and bottom quark mass...
We update the experimental moments for the charm quark as computed in [J. H. Kühn, M. Steinhauser, a...
We update the experimental moments for the charm quark as computed in arXiv:hep-ph/0702103. and used...
In this talk we discuss results of a new extraction of the MS charm quark mass using relativistic QC...
The first value is the “running mass ” mb(µ = mb) in the MS scheme, and the second value is the 1S m...
In this paper we compare recent experimental data for the total cross section σ ( e + e − →hadrons) ...
We determine the MS-bar charm quark mass from a charmonium QCD sum rules analysis. On the theoretica...
We provide a new determination of the charm quark mass using the Highly Improved Staggered Quark (HI...