Content : 1) The leading twist pion wave function, 2) "Improved" QCD sum rules with non-local condensates, 3) Pion and kaon form factors and charmonium decays: theory vs experiment, 4) $\gamma^{*}\gamma\pi^{o}$ - form factor, 5) The new non-local axial anomaly, 6) Cross sections $\gamma\gamma --> \pi^+\pi^- , K^+K^-, K_S K_S $
In the article, we calculate the hadronic coupling constants GD2∗Dπ , GDs2∗DK , GB2∗Bπ , GBs2∗BK wit...
Time-reversal symmetry suppresses electron backscattering in a quantum-spin-Hall edge, yielding quan...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...
We describe the present status of the pion distribution amplitude as it originated from two sources:...
We use general relations between the Transition Distribution Amplitudes (TDAs), entering the descrip...
The pion wave function is computed in the low energy effective theory inspired by the instanton vacu...
The charm quark structure function $F^c_2$ and the longitudinal structure function $F_l^p$ is direct...
We illustrate the general scheme of the Sum Rule (SR) method using 2D Quantum Harmonic Oscillator (2...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...
We derive structure functions for the quasielastic production of octet baryons in neutrino and antin...
We perform a quenched computation of the glue momentum fraction in the pion. Different discretizatio...
We show how the isospin vector and axialvector current spectral functions rho_V and rho_A can be use...
We correct our treatment of decays of the lightest chargino to final states containing the lightest ...
We show that the nonperturbative solution of the SU(2) linear sigma model field theory requires colo...
Special eight-resonance unitary and analytic model of nucleon electromagnetic structure is used to a...
In the article, we calculate the hadronic coupling constants GD2∗Dπ , GDs2∗DK , GB2∗Bπ , GBs2∗BK wit...
Time-reversal symmetry suppresses electron backscattering in a quantum-spin-Hall edge, yielding quan...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...
We describe the present status of the pion distribution amplitude as it originated from two sources:...
We use general relations between the Transition Distribution Amplitudes (TDAs), entering the descrip...
The pion wave function is computed in the low energy effective theory inspired by the instanton vacu...
The charm quark structure function $F^c_2$ and the longitudinal structure function $F_l^p$ is direct...
We illustrate the general scheme of the Sum Rule (SR) method using 2D Quantum Harmonic Oscillator (2...
The part of the proton spin $\Sigma$ carried by $u, d, s$ quarks is calculated in the framework of t...
We derive structure functions for the quasielastic production of octet baryons in neutrino and antin...
We perform a quenched computation of the glue momentum fraction in the pion. Different discretizatio...
We show how the isospin vector and axialvector current spectral functions rho_V and rho_A can be use...
We correct our treatment of decays of the lightest chargino to final states containing the lightest ...
We show that the nonperturbative solution of the SU(2) linear sigma model field theory requires colo...
Special eight-resonance unitary and analytic model of nucleon electromagnetic structure is used to a...
In the article, we calculate the hadronic coupling constants GD2∗Dπ , GDs2∗DK , GB2∗Bπ , GBs2∗BK wit...
Time-reversal symmetry suppresses electron backscattering in a quantum-spin-Hall edge, yielding quan...
Quark mass corrections to the spin partonic structure function g_1(x Q^2) and function F_3(x,Q^2) ar...