FIG. 1: Mueller diagrams[23] for a single inclusive cross section. A bold waving line presents the exact Pomeron Green function of (2), which is the sum of the enhanced diagrams of Fig. 1-b. A zig-zag line corresponds to the exchange of a Reggeon. In Eq. (1) we have introduced two new phenomenological parameters, a$_{IPIP}$ and a$_{IPIR}$ = a$_{IRIP}$ , for the description of hadron emission from the Pomeron and Reggeon. There is an additional dimensional parameter, denoted by Q , which represents the average transverse momentum of the produced minijets. Q$_{0}$Q is the effective mass squared of these minijets, with Q$_{0}$ = 2 GeV (see Ref.[24] for details). Q and Q$_{0}$ are needed to calculate the pseudorapidity η which replaces the rapidity y . The relation between y and η is well known (see, for example, Ref.[24]), with the Jacobian where[1], y ( η, Q ) = 1 2 ln    √ Q 0 Q + Q 2 Q 2 + sinh $^{2}$η + sinh η Q 0 Q + Q 2 Q 2 + sinh $^{2}$η − sinh η   $^{,}$ (3) h ( η, Q ) = cosh η √ Q 0 + Q Q + sinh $^{2}$η . (4) G$_{enh}$ ( y ) g$_{i}$ ( b ) → g$_{i}$ ( b, y ) = g$_{i}$ G$_{enh}$ ( y ) S$_{i}$ ( b ) / (1 + g$_{i}$G$_{enh}$ ( y ) S$_{i}$ ( b )) , (5) S$_{i}$ ( b ) = m 2 i 4 π b m$_{i}$ K$_{1}$ ( m$_{i}$ b ) . (6) In the parametrization of Ref.[1], the value of the Pomeron-particle vertices are large. To compensate, we also sum the semi-enhanced diagrams which contribute to the exact vertex of the Pomeron-particle interaction (see Fig. 1-c). This vertex is equal [25, 26] to 3 Y y 0 − a$_{PP}$ a$_{RP}$ a$_{PR}$ − a) IP IR = b) G 3P = c)