evolution (RGE) are given in Appendix A. In the discussed hybrid setup, the soft terms at the scale of gauge-mediation can be written as Here, ˜ m is the typical scale of the gauge-mediated contribution to the soft terms, which is universal in the limit of neglecting α$_{1}$$_{,}$$_{2}$/α$_{3}$ effects, where α$_{i}$ = g 2 $_{i}$/ (4 π ), and g$_{1}$$_{,}$$_{2}$ ( g$_{3}$ ) denote the gauge couplings of the electroweak sector (strong interaction). Above, the coefficient r ∼ < 1 parameterizes the ratio between the gravity-mediated and the gauge-mediated contri- butions. Gravity-mediation induces also trilinear terms of the form While the gauge-mediated initial conditions are flavor-universal, generically the X$_{q}$$_{A}$ and Z$_{A}$$_{q}$ matrices carry non-trivial flavor structure. It is the goal of this paper to explore the different phenomenology following from different ans¨ atze for the generational structure of the X$_{q}$$_{A}$,Z$_{A}$$_{q}$ matrices. The initial conditions Eqs. (3.1) and (3.2) hold at the high scale m$_{M}$ , while flavor-changing and CP-violating processes restrict the weak scale parameters ( δ q $_{ij}$)$_{NM}$ . Thus, the effect of the RG evolution on the soft terms must be evaluated. Furthermore, the ( δ q $_{ij}$)$_{NM}$ parameters are read off from the low energy soft terms in the basis in which the quark mass matrices and gluino couplings are diagonal, which differs from the flavor basis. The requisite rotation of the squarks leaves the parametric pattern of the X$_{ij}$ and Z$_{ij}$ unchanged. B. The δ q parameters A. High scale M 2 ˜ $_{Q$_{L}$}$( m$_{M}$ ) = ˜ m $^{2}$( 1 + rX$_{q}$$_{L}$ ) , M 2 ˜ $_{D$_{R}$}$( m$_{M}$ ) = ˜ m $^{2}$( 1 + rX$_{d}$$_{R}$ ) , M 2 ˜ $_{U$_{R}$}$( m$_{M}$ ) = ˜ m $^{2}$( 1 + rX$_{u}$$_{R}$ ) . (3.1) A $^{u}$( m$_{M}$ ) = ˜ $_{m}$√$_{r Z}$$_{A}$$_{u}$$_{,}$ A $^{d}$( m$_{M}$ ) = ˜ $_{m}$√$_{r Z}$$_{A}$$_{d}$$_{.}$ (3.2) 8