 Under these premises we can now proceed to choose the parameters \(d\) and \(f\) of the theory, i.e., the localization accuracy and the mean localization frequency. The argument given above suggests how one can choose the parameters in such a way that the quantum predictions for microscopic systems remain fully valid while the embarrassing macroscopic superpositions in measurement-like situations are suppressed in very short times. Accordingly, as a consequence of the unified dynamics governing all physical processes, individual macroscopic objects acquire definite macroscopic properties. The choice suggested in the GRW-model is: