content_image/368617.jpg content_image/368615.jpg content_image/368616.jpg content_image/368614.jpg content_image/368613.jpg content_image/368612.jpg content_image/368610.jpg content_image/368611.jpg
## A. Vanishing A -terms 

We consider anarchical models with vanishing A -terms at the messenger scale: 

Hence, our starting point is Eq. (3.3) with 

We obtain the following flavor parameters, at the m$_{Z}$ -scale ( i = 1 , 2): 

and ( i ̸ = j, j = 1 , 2 , 3): 

where 

<img src='content_image/368617.jpg'>

<img src='content_image/368615.jpg'>

<img src='content_image/368616.jpg'>

<img src='content_image/368614.jpg'>

<img src='content_image/368613.jpg'>

The resulting order of magnitude estimates for the chirality-preserving δ q ij parameters are presented in Table V. The chirality-mixing ( δ q $_{ij}$)$_{LR}$ parameters play no role in constraining SUSY flavor in this scenario. 

By comparing the phenomenological constraints of Table I to the order of magnitude predictions of Table V, we obtain an upper bound on r and find the maximal possible effects in this scenario. The strongest bound on r comes from the neutral Kaon system constraint on 〈 δ d 12 〉 : 

The range corresponds to the same assumptions that enter Eq. (4.3). 

<img src='content_image/368612.jpg'>

The ˆ r$_{i}$ (ˆ r u i ) parameters affect only the δ u i 3 ( δ d i $_{3}$) parameters, and they are bounded only be their definition: 

<img src='content_image/368610.jpg'>

<img src='content_image/368611.jpg'>

