X Z B$_{d}$ B$_{s}$ D 0 d$_{n}$ FN FN 0.002 0.005 0.03 0.02 An FN 0.007 0.002 O (1) 0.01 An An 2 · 10 − 4 5 · 10 − 4 O (10 − $^{10}$) 1 TABLE IX: The maximal size of possible effects in the mixing of B$_{d}$ − B$_{d}$ , B$_{s}$ − B$_{s}$ and D 0 − D 0 for low tan β [Eqs. (4.5), (5.10), (5.20)], normalized to the experimental value, and in the neutron EDM d$_{n}$ [Eqs. (4.9), (5.22)], normalized to the experimental upper bound. FN (An) means that the structure of the corresponding soft terms defined in Eqs. (3.1) and (3.2) is dictated by a Froggatt-Nielsen symmetry (is anarchical). • If the flavor and CP structure of the new physics is anarchical, it is quite possible that its effects will be discovered in CP-violating flavor-diagonal observables rather than in flavor-changing measurements. • If new flavor effects of similar relative sizes are discovered in both third generation ( b or t ) decays and second generation ( c decays), then the new physics is likely to have a flavor structure. Furthermore, this structure may well be related to the standard model one. • A situation where non-MFV effects related to third generation physics are larger (in their relative size) than those related to charm physics requires that the flavor structure of the new physics is not related to the standard model one. It is amusing to note that since the strong suppression of gravity-mediated flavor within full anarchy makes the latter almost MFV-like, it allows for the possibility of a long-lived light stop with macroscopic decay length given a suitable particle spectrum [21]. We conclude that the search for new physics in high-precision flavor experiments and in EDM measurements will be very informative about the underlying, very high scale new physics. It will further allow us to test whether mechanisms such as a Froggatt-Nielsen symmetry dictate all flavor structures or not. 24