content_image/343488.jpg content_image/343489.jpg content_image/343490.jpg content_image/343491.jpg content_image/343492.jpg content_image/343493.jpg content_image/343494.jpg content_image/343495.jpg
(for r$_{3}$ = 3): 

The sensitivity in the D system is slightly modified in comparison to Ref. [7] due to the use of the updated analysis of Ref. [13], see also Table I. 

<img src='content_image/343488.jpg'>

<img src='content_image/343489.jpg'>

<img src='content_image/343490.jpg'>

The mixing amplitudes of the B$_{d,s}$ mesons can be significantly enhanced for low M$_{A}$ 0 and large tan β . By comparing the phenomenological constraints of Eq. (2.4) to the predictions of Table III one finds (for r$_{3}$ = 3, tan β = 30 and M$_{A}$ 0 = 200 GeV): 

<img src='content_image/343491.jpg'>

<img src='content_image/343492.jpg'>

The effects on these systems are maximized when the RGE suppression is minimal. Further details, such as a variant of FN models with holomorphic zeros, where the gravity-mediated contribution to the D 0 − D 0 mixing amplitude can be of O (1), can be found in Ref. [7]. 

## B. A -terms in hybrid FN models 

Going beyond Ref. [7], we investigate here the trilinear A -terms in hybrid models with a FN flavor symmetry. In such scenarios, the A -terms follow the same parametric suppression as the corresponding Yukawa matrices Y . At the high, messenger scale: 

<img src='content_image/343493.jpg'>

Since the A -terms are only similar in texture to the Yukawa matrices, but not proportional to them, rotating to the mass basis leaves the A -terms undiagonalized ( q = u, d ) 

<img src='content_image/343494.jpg'>

The resulting chirality-mixing δ q LR parameters, see Eq. (3.3), are less important for flavor physics than the chirality-preserving δ q LL,RR parameters. If CP-violating, the δ q LR induce a neutron EDM allowed by Eq. (4.3): 

<img src='content_image/343495.jpg'>

where the first value corresponds to x = 1 and a phase suppression in ( δ q $_{11}$)$_{LR}$ of ∼ 0 . 3, and the value in parentheses is obtained for x = 4 and a phase suppression of ∼ 0 . 1. 

