1988
DOI: 10.1063/1.341049
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Thermoelectric properties of lanthanum sulfide with Sm, Eu, and Yb additives

Abstract: The Seebeck coefficient and electrical resistivity have been measured for the La3−x Mx S4 alloys with the Th3 P4 -type structure for M=Sm, Eu, Yb, and x=0.1 to 0.9 in order to determine their potential as high-temperature thermoelectric energy conversion materials. An analysis of the lattice parameters of these alloys suggests that Sm has a valence of 2.2 over the entire composition range. Furthermore, the variation of the Seebeck coefficient and electrical resistivity as a function of electron concentration i… Show more

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Cited by 55 publications
(31 citation statements)
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“…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).…”
Section: Introductionmentioning
confidence: 99%
“…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).…”
Section: Introductionmentioning
confidence: 99%
“…In the last three decades, Si-Ge alloys, 2) several metal chalcogenides, 3,4) transition-metal disilicides [5][6][7] and some boron compounds 8,9) have attracted attention and have been developed as materials for high-temperature thermoelectrics. [10][11][12] However, the abovementioned materials have never been applied practically because of expensive surface protection required to prevent oxidation or vaporization and/or inherent temperature limitation due to phase transformation at high temperatures.…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3][4][5][6][7][8][9][10][11] However, in order to apply these materials to thermoelectric devices for smallscale refrigeration and power generation, it is required to prepare thin films. A majority of the previous studies have been confined to the investigation of bulk materials.…”
Section: Introductionmentioning
confidence: 99%