q ij ( δ q $_{ij}$)$_{LL}$ ( δ q $_{ij}$)$_{RR}$ 〈 δ q ij 〉 d 12 [10 − $^{4}$(3 /r$_{3}$ )] 1 . 2 · 10 − 7 4 · 10 − 6 √ 3 /r$_{3}$ d 13 [0 . 003(3 /r$_{3}$ )] 1 . 2 · 10 − 7 2 · 10 − 5 3 /r$_{3}$ d 23 [0 . 01(3 /r$_{3}$ )] 1 . 2 · 10 − 7 4 · 10 − 5 √ 3 /r$_{3}$ u 12 10 − $^{7}$max { 4 . 8 /r$_{3}$, 1 . 2 } 1 . 2 · 10 − 7 10 − $^{7}$max { 1 . 4 3 /r$_{3}$, 1 . 2 } u 13 [4 · 10 − $^{6}$(3 /r$_{3}$ )] 1 . 2 · 10 − 7 7 · 10 − 7 √ 3 /r$_{3}$ u 23 [4 · 10 − $^{5}$(3 /r$_{3}$ )] 1 . 2 · 10 − 7 2 · 10 − 6 3 /r$_{3}$ TABLE VIII: The order of magnitude upper bounds on ( δ d,u ij )$_{LL,RR}$ and 〈 δ d,u ij 〉 for r/r$_{3}$ ∼ < 1 . 2 · 10 − $^{7}$, obeying the bound of Eq. (5.14) for tan β = 3. Entries in parentheses are independent of r , therefore representing estimates rather than upper bounds. The largest possible contributions to the B$_{d,s}$ mixing amplitudes come from the MFV con- tributions to the ( δ d i $_{3}$)$_{LL}$ ’s. Therefore, the effect is not enhanced for large tan β . We conclude that, for anarchical gravity-mediated contributions to the A -terms, the effects on FCNC processes are negligibly small. In contrast, any improvements in the neutron EDM measurements may either further strengthen the constraints on this framework or discover its effects. Here we explore the implications of A -terms of Yukawa-like texture as in the models with a FN symmetry discussed in Section IV A, specifically, Eq. (4.7), and As concerns the δ q LL,RR parameters, the effect of such A -terms can be described as O ( r ) changes in the RGE coefficients c$_{u}$, c$_{d}$, c$_{uR}$, c$_{dR}$ defined in Eq. (A2); see Eqs. (A6) and (A7). This leads, in turn, to at most O (1) changes in the X$_{q}$$_{A}$ matrices. Therefore, the estimates for the ( δ q $_{ij}$)$_{LL,RR}$ parameters in this scenario vary by at most O (1) from the estimates obtained in Section V A for Z$_{A}$$_{q}$ = 0 at the high scale. As concerns the δ q LR parameters, the parametric suppression of ˜ A q ij can be extracted from 20 ( X$_{q}$$_{A}$ )$_{ij}$ = O (1) , ( Z$_{A}$$_{q}$ )$_{ij}$ ∼ Y q ij ∼ V$_{ij}$m$_{q}$$_{j}$/v$_{q}$. (5.21) C. Yukawa-like A -terms