title: Gd4Ge(3-x)Pn(x) (Pn = P, Sb, Bi, x = 0.5-3): stabilizing the nonexisting Gd4Ge3 binary through valence electron concentration. Electronic and magnetic properties of Gd4Ge(3-x)Pn(x).
abstract: Gd(4)Ge(3-x)Pn(x) (Pn = P, Sb, Bi; x = 0.5-3) phases have been prepared and characterized using X-ray diffraction, wavelength-dispersive spectroscopy, and magnetization measurements. All Gd(4)Ge(3-x)Pn(x) phases adopt a cubic anti-Th(3)P(4) structure, and no deficiency on the Gd or p-element site could be detected. Only one P-containing phase with the Gd(4)Ge(2.51(5))P(0.49(5)) composition could be obtained, as larger substitution levels did not yield the phase. Existence of Gd(4)Ge(2.51(5))P(0.49(5)) and Gd(4)Ge(2.49(3))Bi(0.51(3)) suggests that the hypothetical Gd(4)Ge(3) binary can be easily stabilized by a small increase in the valence electron count and that the size of the p element is not a key factor. Electronic structure calculations reveal that large substitution levels with more electron-rich Sb and Bi are possible for charge-balanced (Gd(3+))(4)(Ge(4-))(3) as extra electrons occupy the bonding Gd-Gd and Gd-Ge states. This analysis also supports the stability of Gd(4)Sb(3) and Gd(4)Bi(3). All Gd(4)Ge(3-x)Pn(x) phases order ferromagnetically with relatively high Curie temperatures of 234-356 K. The variation in the Curie temperatures of the Gd(4)Ge(3-x)Sb(x) and Gd(4)Ge(3-x)Bi(x) series can be explained through the changes in the numbers of conduction electrons associated with  Ge/Sb(Bi) substitution.
authors.affiliation: Department of Chemistry and Chemical Biology, McMaster University, Hamilton, Ontario, L8S 4M1, Canada.
authors.forename: Yan Yin Janice
authors.initials: YY
authors.lastname: Cheung
authors.forename: Volodymyr
authors.initials: V
authors.lastname: Svitlyk
authors.forename: Yurij
authors.initials: Y
authors.lastname: Mozharivskyj