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For small values of tan β , ˆ r = r and Eq. (4.3) applies to ˆ r . Inserting r/r$_{3}$ ∼ < 0 . 03 and r ≤ ˆ r ∼ < 1 into the predictions of Table III, we obtain the upper bounds on the δ q ij presented in Table IV. 

The maximal possible effects in the neutral B$_{d}$, B$_{s}$ and D systems are thus as follows 

