The issue is the expediency of the QCD notions use in the low energy region down to the confinement scale, and, in particular, the efficacy of the QCD invariant coupling \bar{\alpha}_s(Q^2) with a minimal analytic modification in this domain. To this goal, we overview a quite recent progress in application of the ghost-free Analytic Perturbative Theory approach (with no adjustable parameters) for QCD in the region below 1 GeV. Among them the Bethe--Salpeter analysis of the meson spectra and spin-dependent (polarization) Bjorken sum rule. The impression is that there is a chance for the theoretically consistent and numerically correlated description of hadronic events from Z_0 till a few hundred MeV scale by combination of analytic pQCD and ...
There are indications of a faith transition in QCD: The strong coupling may freeze at a sufficiently...
We consider an extension of the one-nucleon sector of baryon chiral perturbation theory beyond the l...
Analytic versions of QCD are those whose coupling αs(Q²) does not have the unphysical Landau singula...
Part I is devoted to the extraction of the QCD coupling from a bound state approach at low energy sc...
An elegant and more precise formula for the 3-loop perturbative QCD coupling is discussed. It improv...
A comprehensive review is presented of the progress made in further developing the ghost-free Analyt...
A comprehensive review is presented of the progress made in further developing the ghost-free Analyt...
As is known from QED, a possible solution to the ghost-pole trouble can be obtained by imposing the ...
AbstractThe QCD running coupling αs(Q2) sets the strength of the interactions of quarks and gluons a...
The low energy behavior of a recently proposed model for the massive analytic running coupling of QC...
We test the recently proposed “Massive” Perturbation Theory (MPT) for the description of the Γ(1)p-n...
We discuss the new model expression $\bar{\alpha}_{an}(Q~2)$ recently obtained for the QCD running c...
In quantum theory, physical amplitudes are usually presented in the form of Feynman perturbation ser...
Within the ghost-free Analytic Perturbation Theory (APT), devised in the last decade for low energy ...
Experimental data obtained for the polarized Bjorken sum rule (BSR) $$\Gamma _1^{p-n}(Q^2)$$ are fit...
There are indications of a faith transition in QCD: The strong coupling may freeze at a sufficiently...
We consider an extension of the one-nucleon sector of baryon chiral perturbation theory beyond the l...
Analytic versions of QCD are those whose coupling αs(Q²) does not have the unphysical Landau singula...
Part I is devoted to the extraction of the QCD coupling from a bound state approach at low energy sc...
An elegant and more precise formula for the 3-loop perturbative QCD coupling is discussed. It improv...
A comprehensive review is presented of the progress made in further developing the ghost-free Analyt...
A comprehensive review is presented of the progress made in further developing the ghost-free Analyt...
As is known from QED, a possible solution to the ghost-pole trouble can be obtained by imposing the ...
AbstractThe QCD running coupling αs(Q2) sets the strength of the interactions of quarks and gluons a...
The low energy behavior of a recently proposed model for the massive analytic running coupling of QC...
We test the recently proposed “Massive” Perturbation Theory (MPT) for the description of the Γ(1)p-n...
We discuss the new model expression $\bar{\alpha}_{an}(Q~2)$ recently obtained for the QCD running c...
In quantum theory, physical amplitudes are usually presented in the form of Feynman perturbation ser...
Within the ghost-free Analytic Perturbation Theory (APT), devised in the last decade for low energy ...
Experimental data obtained for the polarized Bjorken sum rule (BSR) $$\Gamma _1^{p-n}(Q^2)$$ are fit...
There are indications of a faith transition in QCD: The strong coupling may freeze at a sufficiently...
We consider an extension of the one-nucleon sector of baryon chiral perturbation theory beyond the l...
Analytic versions of QCD are those whose coupling αs(Q²) does not have the unphysical Landau singula...