The idea of partons and the utility of using light-cone gauge in QCD are introduced. Saturation of quark and gluon distributions are discussed using simple models and in a more general context. The Golec-Biernat W\usthoff model and some simple phenomenology are described. A simple, but realistic, equation for unitary, the Kovchegov equation, is discussed, and an elementary derivation of the JIMWLK equation is given
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
Exclusive photoproduction of heavy quarkonia in high-energy ultraperipheral ion-ion interactions (ga...
Partons are defined as the quanta in a Fock space description of a hadron. Gluon saturation is descr...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
The equation of state for quark-gluon plasma is obtained, being valid for arbitrary values of the co...
We present the perturbative QCD calculation of diffractive $D_s$ production in charged current deep ...
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...
Longitudinal and transverse quark momentum distributions in the nucleon are calculated from a phenom...
Approximate relations among transverse momentum dependent quark distribution functions are establish...
A possibility of semiphenomenological description of vacuum effects in QCD quantized on the Light Fr...
Dynamical chiral symmetry breaking (DCSB) is one of the keystones of low-energy hadronic phenomena. ...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We present a model calculation of the generalized parton distributions where the nucleon is describe...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
Exclusive photoproduction of heavy quarkonia in high-energy ultraperipheral ion-ion interactions (ga...
Partons are defined as the quanta in a Fock space description of a hadron. Gluon saturation is descr...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
The equation of state for quark-gluon plasma is obtained, being valid for arbitrary values of the co...
We present the perturbative QCD calculation of diffractive $D_s$ production in charged current deep ...
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...
Longitudinal and transverse quark momentum distributions in the nucleon are calculated from a phenom...
Approximate relations among transverse momentum dependent quark distribution functions are establish...
A possibility of semiphenomenological description of vacuum effects in QCD quantized on the Light Fr...
Dynamical chiral symmetry breaking (DCSB) is one of the keystones of low-energy hadronic phenomena. ...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We present a model calculation of the generalized parton distributions where the nucleon is describe...
We argue that the difference between the structure functions corresponding to deep inelastic scatter...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
Exclusive photoproduction of heavy quarkonia in high-energy ultraperipheral ion-ion interactions (ga...