Abstract
Citations in the original article are corrupted due to error made by Editors QUARKS-2018. See the Full text with correct citations in PDF file.
Highlights
Full text with correct citations follows. It is well-known that the masses of charm, bottom and top-quarks are one of the most important QCD parameters, which are relevant for processing different data, obtained at LHC and
The first ones are determined by the position of pole of the renormalized fermion propagator at Minkowskian region k2 = Mq2
Mq(μ2) are the running masses of heavy quarks, normalized at the Minkowskian scale μ2, as(μ2) = αs(μ2)/π is the renormalized QCD coupling constant in the MS-scheme, s is the energy time-like variable
Summary
It is well-known that the masses of charm, bottom and top-quarks are one of the most important QCD parameters, which are relevant for processing different data, obtained at LHC and. The presented in Sec. comparison of five- and six-loop estimates, obtained within both approaches, demonstrates that the above mentioned approximate equality remains true at the 5 and 6-loops level as well This demonstrates compatibility of the estimates for heavy quark mass relations coefficients, obtained by applying ECH-inspired procedure both in the Euclidean and Minkowskian regions
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