Processes of phase separations into B2+DO
3 or A2+DO
3 at 873 K in Fe-Si-Ge ternary ordering alloys were investigated by TEM observations of microstructure and the free energies of all the relevant phases were evaluated. Sequences of phase separation from the A2 or B2 single phase state into the B2+DO
3 or A2+DO
3 equilibrium state were classified into five types. (1) In the alloys near the phase boundary B2/B2+DO
3, continuous ordering from A2 to B2 occurs at first and then the DO
3 phase is formed inside the B2 phase domains. (2) In the alloys near the phase boundary B2+DO
3/DO
3, continuous ordering from B2 to DO
3 occurs at first and then the B2 phase is formed on the antiphase boundary of the DO
3 phase. (3) In the alloys near the phase boundary A2/A2+DO
3, the phase separation of A2 into A2+DO
3 occurs directly without through any intermediate state. (4) In the alloys whose compositions are located in the centre area of the A2+DO
3 field, phase decomposition from the B2 into B2+DO
3 arises, followed by the phase separation into A2+DO
3. (5) In the alloys near the boundary A2+DO
3/DO
3, continuous ordering from the B2 to DO
3 phase occurs at first and then A2 phase is formed on the antiphase boundaries of DO
3 phase. These sequences of phase separations could be explained from the hierarchy of free energies among the A2, B2 and DO
3 phases evaluated on the basis of the Bragg-Williams-Gorsky approximation.
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