In this study, we examine the effects of heating, nucleation, cooling, and reheating on the thermal properties and structure of metallocene isotactic polypropylene (m-iPP) that had been prepared initially in a standard state containing nearly equal amounts of the crystallographic ␣ and ␥ phases. Heat treatment was achieved through partial melting and annealing by the heating of samples to self-nucleation temperatures (T n 's) that spanned and exceeded the entire range of melting of the standard state, from 122 to 160°C. The relative amounts of ␣ and ␥ crystals are determined from the area under the unique wide-angle X-ray reflections. The lower and upper endotherms are caused by the melting of ␥ and ␣ crystals, respectively. Four distinct regions of T n were identified on the basis of the thermal and structural parameters of m-iPP. In region I, T n is below the peak melting temperature of the ␥ phase. Here, ␥ crystals are annealed and ␣ crystals are barely affected by T n . In region II, T n is above the peak of the lower endotherm but below the peak of the upper endotherm. ␥ crystals melt, and ␣ crystals anneal. In both regions I and II, the portion of the sample melted at T n recrystallizes epitaxially with existing parent ␣ lamellae as the substrates, and the amount of ␣ always exceeds the amount of ␥. In region III, T n is above the peak of the upper endotherm, and all ␥ crystals and some or all ␣ crystals are melted at T n . The number of ␣-crystal nuclei steadily decreases as T n increases, causing systematic depression of the crystallization and melting temperatures seen during cooling. Finally, in region IV, T n exceeds the upper endotherm, and only small self-nuclei or heterogeneous nuclei remain. Recrystallization is now suppressed to lower temperatures. For regions III and IV, a crossover behavior in the relative amounts of ␣ and ␥ is observed during cooling from T n . Because of the effective nucleating ability of ␣ toward ␥, as the temperature drops, the amount of ␥ increases and then exceeds the amount of ␣. With subsequent reheating, the reverse crossover occurs because of the lower melting point of ␥.