Add to ORKGOn the basis of the target mass corrections to structure functions of deep-inelastic scattering of leptons, we evaluate effective nucleon mass that turns out to be twice M_{nucl.} for deep-inelastic scattering on the nucleus target and equals M_{nucl.} for the hydrogen target
We compute in the heavy quark effective theory the soft coefficient D_2 entering the resummation of ...
The semiclassical method for description of the radiative strength function is used for asymmetric n...
A simple matching procedure is proposed to extract constraints on effective meson theories. In this ...
We analyze experimental data of nuclear structure function ratios $F_2^A/F_2^D$ for obtaining optimu...
We calculate the nucleon parameters in isospin symmetric and asymmetric nuclear matter using the QCD...
After a brief review of the experimental results obtained in deep inelastic lepton-nucleon scatterin...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
We analyze nuclear effects in the deep inelastic scattering on deuteron in the framework of the cova...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...
A relation among the effective nucleon mass $M^*$, the incompressibility $K$ and the effective $\sig...
The charm quark structure function $F^c_2$ and the longitudinal structure function $F_l^p$ is direct...
The $F_{2}$, $F_{G}$, $R=F_{L}/F_{T}$ proton structure functions are derived in the QCD dipole pictu...
A QCD sum rule calculation of Balistky and Ji on the spin content of the nucleon is done with a diff...
Precise measurements of polarized electro-production and Drell-Yan in the deep inelastic limit will ...
Two photon decay widths of the $J^P = O^+$ scalar mesons $a_{0} (980)$, $f_{0}(980)$, $f_{0}(1370)$ ...
We compute in the heavy quark effective theory the soft coefficient D_2 entering the resummation of ...
The semiclassical method for description of the radiative strength function is used for asymmetric n...
A simple matching procedure is proposed to extract constraints on effective meson theories. In this ...
We analyze experimental data of nuclear structure function ratios $F_2^A/F_2^D$ for obtaining optimu...
We calculate the nucleon parameters in isospin symmetric and asymmetric nuclear matter using the QCD...
After a brief review of the experimental results obtained in deep inelastic lepton-nucleon scatterin...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
We analyze nuclear effects in the deep inelastic scattering on deuteron in the framework of the cova...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...
A relation among the effective nucleon mass $M^*$, the incompressibility $K$ and the effective $\sig...
The charm quark structure function $F^c_2$ and the longitudinal structure function $F_l^p$ is direct...
The $F_{2}$, $F_{G}$, $R=F_{L}/F_{T}$ proton structure functions are derived in the QCD dipole pictu...
A QCD sum rule calculation of Balistky and Ji on the spin content of the nucleon is done with a diff...
Precise measurements of polarized electro-production and Drell-Yan in the deep inelastic limit will ...
Two photon decay widths of the $J^P = O^+$ scalar mesons $a_{0} (980)$, $f_{0}(980)$, $f_{0}(1370)$ ...
We compute in the heavy quark effective theory the soft coefficient D_2 entering the resummation of ...
The semiclassical method for description of the radiative strength function is used for asymmetric n...
A simple matching procedure is proposed to extract constraints on effective meson theories. In this ...