content_image/343349.jpg content_image/343350.jpg content_image/343351.jpg content_image/343343.jpg content_image/343344.jpg content_image/343345.jpg content_image/343346.jpg
<img src='content_image/343349.jpg'>

<img src='content_image/343350.jpg'>

<img src='content_image/343351.jpg'>

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 

<img src='content_image/343343.jpg'>

<img src='content_image/343344.jpg'>

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 

<img src='content_image/343345.jpg'>

where[1], 

<img src='content_image/343346.jpg'>

