the small precipitate clusters can be formed locally using the theoretical arguments derived we can find the designated temperature where the desirable density and size distribution of the semiconductor nanocrystallite can be obtained the means to induce the spontaneous homogeneous nucleation is important in order to produce a uniform spatial distribution of the semiconductor nuclei pure homogeneous nucleation may not exist in reality the closest means would be sending the shock wave through the under cooled solution for example one can use interferencing acoustic waves to induce higher probabilities for nucleus formation at high intensity interference nodes within the bulk of the solution this increases the overall mean cluster size within a narrow size distribution we know that when the cluster size is greater than the critical value the cluster becomes stable ideally we can keep the glass at t2 until the equilibrium phase separation condition is obtained however it may take too long we can keep the glass at t2 for a period of time d 39 2 so that the number density of the precipitates is stable d 39 2 can be derived by assuming an acceptable margin of the precipitates size u03b4x upon the critical nuclei size at temperature t2 for instance if u03b4x 0 2 r then d 39 2 u02dc 0 04r 2 d where r the critical nuclei.