TY - JOUR
T1 - Flux synthesis, structure and physical properties of new pseudo-binary REAl3-xGex compounds
AU - Zhuravleva, Marina A.
AU - Rangan, K. Kasthuri
AU - Lane, Melissa
AU - Brazis, Paul
AU - Kannewurf, C. R.
AU - Kanatzidis, Mercouri G.
N1 - Funding Information:
Financial support from the Department of Energy (Grant # DE-FG02-99ER45793) is gratefully acknowledged.
PY - 2001/3/2
Y1 - 2001/3/2
N2 - New compounds in the system RE-Al-Ge (RE = Tb, Gd, Ho) were prepared in molten aluminum. Large, (up to 5 mm) single crystals of new pseudo-binary phases GdAl3-xGex, (x = 0.1), TbAl3-xGex, (x = 0.3), and HoAl3-xGex, (x = 0.2) were recovered in high yield. The crystal structures were refined by single crystal X-ray diffraction techniques, and found to vary as a function of rare-earth element. Thus, GdAl3-xGex crystallizes in the Ni3Sn structure type (P63/mmc) of GdAl3. For the TbAl3-xGex the BaPb3 structure type (R-3m) is adopted, as it is for TbAl3. In the case of HoAl3-xGex, the structure type of HoAl3 is not stabilized, and the compound crystallizes in the BaPb3 structure (R-3m). Crystal data: GdAl3-xGex a = 6.3115(4) angstroms, c = 4.6052(4) angstroms, V = 158.87(2) angstroms3, P63/mmc (No. 194, Z = 2); TbAl3-xGex a = 6.1956(9) angstroms, c = 21.025(4) angstroms, V = 698.9(2) angstroms3, R-3m (No. 166, Z = 9); HoAl3-xGex a = 6.1579(10) angstroms, c = 21.062(5) angstroms, V = 691.7(2) angstroms3, R-3m (No. 166, Z = 9). Charge transport properties indicate that these materials are good metallic conductors. At low temperatures they order antiferromagnetically, whereas above approximately 50 K they are Curie-Weiss paramagnets. The temperature of maximum magnetic susceptibility (Tmax) is 5.93 K, 18.8 K, and 24.0 K for HoAl2.8Ge0.2, TbAl2.7Ge0.3, and GdAl2.9Ge0.1 respectively.
AB - New compounds in the system RE-Al-Ge (RE = Tb, Gd, Ho) were prepared in molten aluminum. Large, (up to 5 mm) single crystals of new pseudo-binary phases GdAl3-xGex, (x = 0.1), TbAl3-xGex, (x = 0.3), and HoAl3-xGex, (x = 0.2) were recovered in high yield. The crystal structures were refined by single crystal X-ray diffraction techniques, and found to vary as a function of rare-earth element. Thus, GdAl3-xGex crystallizes in the Ni3Sn structure type (P63/mmc) of GdAl3. For the TbAl3-xGex the BaPb3 structure type (R-3m) is adopted, as it is for TbAl3. In the case of HoAl3-xGex, the structure type of HoAl3 is not stabilized, and the compound crystallizes in the BaPb3 structure (R-3m). Crystal data: GdAl3-xGex a = 6.3115(4) angstroms, c = 4.6052(4) angstroms, V = 158.87(2) angstroms3, P63/mmc (No. 194, Z = 2); TbAl3-xGex a = 6.1956(9) angstroms, c = 21.025(4) angstroms, V = 698.9(2) angstroms3, R-3m (No. 166, Z = 9); HoAl3-xGex a = 6.1579(10) angstroms, c = 21.062(5) angstroms, V = 691.7(2) angstroms3, R-3m (No. 166, Z = 9). Charge transport properties indicate that these materials are good metallic conductors. At low temperatures they order antiferromagnetically, whereas above approximately 50 K they are Curie-Weiss paramagnets. The temperature of maximum magnetic susceptibility (Tmax) is 5.93 K, 18.8 K, and 24.0 K for HoAl2.8Ge0.2, TbAl2.7Ge0.3, and GdAl2.9Ge0.1 respectively.
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U2 - 10.1016/S0925-8388(00)01411-0
DO - 10.1016/S0925-8388(00)01411-0
M3 - Article
AN - SCOPUS:0035277425
SN - 0925-8388
VL - 316
SP - 137
EP - 145
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
IS - 1-2
ER -