We consider the one-chain term in a skeleton expansion for Euclidean QCD observables. Focusing on the particular example of the Adler D function, we show that although there is a Landau pole in the coupling at Q^2=\Lambda^2 which renders fixed-order perturbative results infinite, the Landau pole is absent in the all-orders one-chain result. In this approximation one has finiteness and continuity at Q^2=\Lambda^2, and a smooth freezing as Q^2 decreases to 0
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We develop a new mathematical method of extraction of nonperturbative corrections in QCD. The main a...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...
In these lectures we give a concise introduction to the ideas of renormalon calculus in QED and QCD....
The 't Hooft model for the two-dimensional QCD in the limit of infinite number of colours is studied...
The monopole order parameter of QCD is computed in terms of gauge invariant field strength correlato...
Because present Monte Carol algorithms for lattice QCD may become trapped in a given topological cha...
If QCD is renormalized by minimal subtraction (MS), at higher orders, the strong coupling constant a...
The Gell-Mann - Low function \beta(g) in QCD (g=g0^2/16\pi^2 where g0 is the coupling constant in th...
The equation of state for quark-gluon plasma is obtained, being valid for arbitrary values of the co...
A possibility of semiphenomenological description of vacuum effects in QCD quantized on the Light Fr...
A simple but effective method for regularization-renormalization (R-R) is proposed for handling the ...
Effects of dispersion of the chromoelectric field of the flux tube on the string-breaking distance a...
We consider the leading one-chain term in a skeleton expansion for QCD observables and show that for...
We suggest that the QCD corrections to QED calculations may be probed through optical experiments in...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We develop a new mathematical method of extraction of nonperturbative corrections in QCD. The main a...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...
In these lectures we give a concise introduction to the ideas of renormalon calculus in QED and QCD....
The 't Hooft model for the two-dimensional QCD in the limit of infinite number of colours is studied...
The monopole order parameter of QCD is computed in terms of gauge invariant field strength correlato...
Because present Monte Carol algorithms for lattice QCD may become trapped in a given topological cha...
If QCD is renormalized by minimal subtraction (MS), at higher orders, the strong coupling constant a...
The Gell-Mann - Low function \beta(g) in QCD (g=g0^2/16\pi^2 where g0 is the coupling constant in th...
The equation of state for quark-gluon plasma is obtained, being valid for arbitrary values of the co...
A possibility of semiphenomenological description of vacuum effects in QCD quantized on the Light Fr...
A simple but effective method for regularization-renormalization (R-R) is proposed for handling the ...
Effects of dispersion of the chromoelectric field of the flux tube on the string-breaking distance a...
We consider the leading one-chain term in a skeleton expansion for QCD observables and show that for...
We suggest that the QCD corrections to QED calculations may be probed through optical experiments in...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We develop a new mathematical method of extraction of nonperturbative corrections in QCD. The main a...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...