The transition form factor, decay width and charge form factor of pion are calculated within the model of induced nonlocal quark currents based on the assumption that the nonperturbative QCD vacuum can be characterized by a homogeneous (anti-)self-dual gluon field. It is shown that the interaction of the quark spin with the vacuum gluon field, being responsible in the model for the chiral symmetry breaking and the spectrum of light mesons, can also play the decisive role in forming the transition form factor and two-photon decay width. Asymptotic behavior of quark loops in the presence of the background gluon field for large momentum transfer is discussed
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
We investigate the interplay of chiral and heavy quark symmetries by using the NJL quark model. Heav...
We show that for small x and in the double logarithmic approximation (DLA) g_2 can be expressed thro...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
We use the method of QCD sum rules to investigate the isospin symmetry breaking of K and K* mesons. ...
The charm quark structure function $F^c_2$ and the longitudinal structure function $F_l^p$ is direct...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
An approach for a unified description of the nucleon electromagnetic form factors in spacelike and t...
A simple matching procedure is proposed to extract constraints on effective meson theories. In this ...
The $Q \bar{Q}$ semirelativistic interaction in QCD can be expressed in terms of the Wilson loop and...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
We investigate the interplay of chiral and heavy quark symmetries by using the NJL quark model. Heav...
We show that for small x and in the double logarithmic approximation (DLA) g_2 can be expressed thro...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
We use the method of QCD sum rules to investigate the isospin symmetry breaking of K and K* mesons. ...
The charm quark structure function $F^c_2$ and the longitudinal structure function $F_l^p$ is direct...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
An approach for a unified description of the nucleon electromagnetic form factors in spacelike and t...
A simple matching procedure is proposed to extract constraints on effective meson theories. In this ...
The $Q \bar{Q}$ semirelativistic interaction in QCD can be expressed in terms of the Wilson loop and...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...