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The Gd-Ti phase diagram in [Massalski2] was redrawn from [1987Mur], as shown with solid lines in Fig. 1. The miscibility gap in the liquid phase was estimated based on scarce thermodynamic data.
[2010Sch] determined the miscibility gap by means of electromagnetic levitation experiments. The result is shown with a dashed line in Fig. 1. The critical temperature and composition are approximately 1580 °C and 80 at.% Ti, respectively. The location of the miscibility gap is in good agreement with [1987Mur] on the Gd-rich side, but very different on the Ti-rich side. Because it is unlikely that the critical composition of a simple one-peak miscibility gap is displaced to 80 at.% [1993Oka2], it is possible that the peak in this case is one of a two-peak miscibility gap (the other peak is not fully developed due to asymmetry in the interaction parameter) [1993Oka1]. Then a concave segment may appear in the middle section of the miscibility gap instead of a simple convex form shown in Fig. 1. This is not inconsistent with the experimental data reported by [2010Sch]. A new thermodynamic assessment is required.
References
J.L. Murray, The Gd-Ti (Gadolinium-Titanium) System, Phase Diagrams of Binary Titanium Alloys, J.L. Murray, Ed., ASM International, Metals Park, OH, 1987, p 225-228
H. Okamoto, A Two-Peak Miscibility Gap, J. Phase Equilib., 1993, 14(3), p 336-339
H. Okamoto and T.B. Massalski, Guidelines for Binary Phase Diagram Assessment, J. Phase Equilib., 1993, 14(3), p 316-335
S. Schmitz, H.G. Lindenkreuz, N. Mattern, W. Loser, and B. Buchner, Liquid Phase Separation in Gd-Ti and Gd-Zr Melts, Intermetallics, 2010, 18, p 1941-1945
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Okamoto, H. Gd-Ti (Gadolinium-Titanium). J. Phase Equilib. Diffus. 33, 422 (2012). https://doi.org/10.1007/s11669-012-0080-6
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DOI: https://doi.org/10.1007/s11669-012-0080-6