  We point out that there exists an absolute lower bound on sin 2\beta in all
models with minimal flavour violation (MFV), that do not have any new operators
beyond those present in the Standard Model and in which all flavour changing
transitions are governed by the CKM matrix with no new phases beyond the KM
phase. This bound depends only on V_{cb}, V_{ub} and the hadronic parameters
\hat B_K, F_{B_d}\sqrt{\hat B_d} and \xi relevant for the CP-violating
parameter \varepsilon and the B^0_{d,s}-\bar B^0_{d,s} mixings. Performing a
simple scanning over the present ranges of these parameters we find sin
2\beta\ge 0.34. We illustrate how this bound could become stronger when our
knowledge of the parameters in question improves and when the upper bound on
the B^0_{s}-\bar B^0_{s} mixing ((\Delta M)_s) will be experimentally known.
Provided the future accurate measurements of sin 2\beta through the CP
asymmetry in B_d^0(\bar B_d^0)\to \psi K_S will confirm the low values recently
reported by BaBar and Belle, there is a likely possibility that this class of
models will be excluded. This would firmly imply the necessity of new
CP-violating phases and/or new effective operators in the weak effective
Hamiltonians for K^0-\bar K^0 and B^0_{d,s}-\bar B^0_{d,s} mixings. We also
point out that within the MFV models there exists also an absolute lower bound
on the angle \gamma. We find \sin\gamma\ge 0.24. This lower bound could become
stronger in the future.
