Abstract
We solve a unified integral equation to obtain the and dependence of the gluon distribution of a proton in the small regime; where and are the longitudinal momentum fraction and the transverse momentum of the gluon probed at a scale . The equation generates a gluon with a steep behaviour, with , and a distribution which broadens as decreases. We compare our solutions with, on the one hand, those that we obtain using the double-leading-logarithm approximation to Altarelli-Parisi evolution and, on the other hand, to those that we determine from the BFKL equation.
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