AbstractWe present first calculations of the fluctuating gluon distribution in a proton as a function of impact parameter and rapidity employing the functional Langevin form of the JIMWLK renormalization group equation. We demonstrate that when including effects of confinement by screening the long range Coulomb field of the color charges, the evolution is unitary. The large-x structure of the proton, characterized by the position of three valence quarks, retains an effect on the proton shape down to very small values of x. We determine the dipole scattering amplitude as a function of impact parameter and dipole size and extract the rapidity evolution of the saturation scale and the proton radius at fixed QCD coupling
Determining the inner structure of protons and nuclei in terms of their fundamental constituents has...
Employing the representation of the experimental data on deep inelastic electron-proton scattering (...
AbstractThe gluon distribution is dominated by the hard pomeron at small x and all Q2, with no soft-...
AbstractWe present first calculations of the fluctuating gluon distribution in a proton as a functio...
The energy evolution of the fluctuating proton structure is studied by solving the JIMWLK renormaliz...
Boroun GR, Kuroda M, Schildknecht D. The Proton Gluon Distribution from the Color Dipole Picture. ar...
We develop a model to compute high-energy reactions of hadrons and photons. The perturbative interac...
The differential and the total cross sections in high energy hadron-proton interactions give a beaut...
The differential and the total cross sections in high energy hadron-proton interactions give a beaut...
The differential and the total cross sections in high energy hadron-proton interactions give a beaut...
In the semiclassical approach, inclusive and diffractive quark and gluon distributions are expressed...
The color dipole formulation provides an intuitive picture of hard processes in high energy scatteri...
We argue that the amount of baryon stopping observed in the central rapidity region of heavy ion col...
Impact parameter dependent dipole models are ideal tools for investigating the spatial structure of ...
The gluon radius of the proton is expected to increase at small gluon momentum fractions $x$, an eff...
Determining the inner structure of protons and nuclei in terms of their fundamental constituents has...
Employing the representation of the experimental data on deep inelastic electron-proton scattering (...
AbstractThe gluon distribution is dominated by the hard pomeron at small x and all Q2, with no soft-...
AbstractWe present first calculations of the fluctuating gluon distribution in a proton as a functio...
The energy evolution of the fluctuating proton structure is studied by solving the JIMWLK renormaliz...
Boroun GR, Kuroda M, Schildknecht D. The Proton Gluon Distribution from the Color Dipole Picture. ar...
We develop a model to compute high-energy reactions of hadrons and photons. The perturbative interac...
The differential and the total cross sections in high energy hadron-proton interactions give a beaut...
The differential and the total cross sections in high energy hadron-proton interactions give a beaut...
The differential and the total cross sections in high energy hadron-proton interactions give a beaut...
In the semiclassical approach, inclusive and diffractive quark and gluon distributions are expressed...
The color dipole formulation provides an intuitive picture of hard processes in high energy scatteri...
We argue that the amount of baryon stopping observed in the central rapidity region of heavy ion col...
Impact parameter dependent dipole models are ideal tools for investigating the spatial structure of ...
The gluon radius of the proton is expected to increase at small gluon momentum fractions $x$, an eff...
Determining the inner structure of protons and nuclei in terms of their fundamental constituents has...
Employing the representation of the experimental data on deep inelastic electron-proton scattering (...
AbstractThe gluon distribution is dominated by the hard pomeron at small x and all Q2, with no soft-...