Abstract

The phase equilibria, A2/B2 and B2/L2 1 order–disorder transitions and ferromagnetic/paramagnetic transition on the Co–Fe side of the Co–Fe–Ga system were examined by electron probe microanalysis (EPMA), differential scanning calorimetric (DSC) measurement and vibrating sample magnetometer (VSM). The equilibrium compositions of interrelations mainly among γ (A1: disordered fcc-Co), α (A2: disordered bcc-Fe), β (B2: ordered bcc-CoGa or FeGa) and β′ (L2 1 or D0 3: ordered bcc-Co 2FeGa or Fe 3Ga) phases were determined using diffusion couples and two-phase bulk specimens. It was confirmed that a bcc single-phase region composed of α, β and β′ at 700–1000° C exists in a wide composition range and that the ferromagnetic region appearing on the Co–Fe side extends to the center of the Gibbs triangle with decreasing temperature. On the other hand, the β′ phase appears along the Fe 3Ga–Co 3Ga section and the maximal critical temperature of the B2/L2 1 order–disorder transformation was determined to be 825 °C at a stoichiometric composition expressed as Co 2FeGa. The obtained phase diagram was examined in comparison with that of the Co–Fe–Al system.

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