Abstract

Saturation in deep inelastic scattering (DIS) and deeply virtual Compton scattering (DVCS) is associated with a phase transition between the partonic gas, typical of moderate xx and Q2Q^2, and partonic fluid appearing at increasing Q2Q^2 and decreasing Bjorken xx. In the statistical interpretation of DIS, the large-x,(1−x)nx,(1-x)^n factor in the SF is associated with a statistical distribution (perfect gas), while the low-xx, Regge behaved factor xb(Q2)x^{b(Q^2)} produces deviations from the perfect gas and ultimately leads to a gas-liquid phase transition. In this paper we do not intend to propose another parametrization of the structure function; instead we suggest a new insight into the internal structure of the nucleon, as seen in DIS, and its connection with that revealed in high-energy nucleons and heavy-ion collisions.

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