“…In particular, the chalcogenides crystallizing with the cubic Th3P 4 structure have received a great deal of attention because the solidsolution compositions extending from Ln2X 3 to Ln3X 4 have this structure and the physical parameters can be varied continuously as the cation vacancies in Ln2X 3 are filled to form the end member Ln3X4. The cation vacancies can be filled with the same or other rareearth elements as well as a great number of non-rareearth metals (Carter, Miller & Ryan, 1961;Taher & Gruber, 1981;Nakahara, Tschetter, Beaudry, Takeshita & Gschneidner, 1986). The published phase diagram of Gd-Te shows such a solid-solution region, Gd2Te3-Gd3Te 4, and electrical resistivity and Seebeck coefficients have been reported (Zargaryan & Abrikosov, 1967;Reid, Matson, Miller & Himes, 1964).…”