In the KLN model, heavy quark masses in the Bjorken variable shift where saturation appears, with protons losing visible saturation and nuclei retaining it at x around 10^-6 and large dipole sizes.
Measuring the Gluon Density in e + A Collisions: KLN CGC, DGLAP Glauber, or Neither?
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abstract
We predict readily experimentally measurable differences in the diffractive cross section in the coherent exclusive photoproduction of J/psi mesons in e + A collisions at eRHIC and LHeC energies for nuclear gluon distributions assumed to 1) evolve in x with DGLAP dynamics and have a spatial distribution proportional to the Glauber nuclear thickness function and 2) evolve in x and b according to the KLN prescription of CGC dynamics. We find that CGC physics predicts that the nuclear gluon density widens significantly as a function of x yielding diffractive peaks and minima that evolve dramatically with x; on the other hand the DGLAP Glauber distribution yields peaks and minima constant in x. We also find that the dipole cross section at the level of two gluon exchange within the KLN parameterization of the CGC satisfies the black disk limit whereas this limit is violated when DGLAP evolution is used; the normalization of the diffractive cross section grows more slowly in x by several orders of magnitude when using the KLN parameterization as compared to the result when employing DGLAP evolution.
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Effects of heavy quarks in the dipole cross section with the KLN model
In the KLN model, heavy quark masses in the Bjorken variable shift where saturation appears, with protons losing visible saturation and nuclei retaining it at x around 10^-6 and large dipole sizes.