TY - JOUR
T1 - Physical properties of GdFe2(AlxZn 1-x)20
AU - Ni, N.
AU - Jia, S.
AU - Samolyuk, G. D.
AU - Kracher, A.
AU - Sefat, A. S.
AU - Bud'Ko, S. L.
AU - Canfield, P. C.
PY - 2011
Y1 - 2011
N2 - The high ferromagnetic ordering temperature of the dilute, rare-earth-bearing, intermetallic compound GdFe2Zn20 has been understood as being the consequence of the Gd3+ moment being embedded in a nearly ferromagnetic Fermi liquid. To test this understanding in detail, single crystals of the pseudoternary series GdFe2(Al xZn1-x)20 (x≤0.122) and YFe 2(AlxZn1-x)20 (x≤0.121) were grown out of Zn-rich solution. Magnetization, heat capacity, and resistivity measurements show that, with Al doping, the ferromagnetic phase transition temperatures of the GdFe2(AlxZn1-x) 20 compounds decrease from 86 K (x= 0) to 10 K (x= 0.122); for the nonmagnetic analog, the YFe2(AlxZn1-x) 20 series, the Stoner enhancement factor Z decreases from 0.88 (x= 0) to 0.35 (x= 0.121) in a similar manner. Tight-binding linear-muffin-tin orbital atomic-sphere approximation band structure calculations are used to rationalize this trend. These results, together with the earlier studies of the R(Fe 1-xCox)2Zn20 (R= Gd and Y) series, clearly highlight the importance of band filling and the applicability of even a simple, rigid-band model to these compounds.
AB - The high ferromagnetic ordering temperature of the dilute, rare-earth-bearing, intermetallic compound GdFe2Zn20 has been understood as being the consequence of the Gd3+ moment being embedded in a nearly ferromagnetic Fermi liquid. To test this understanding in detail, single crystals of the pseudoternary series GdFe2(Al xZn1-x)20 (x≤0.122) and YFe 2(AlxZn1-x)20 (x≤0.121) were grown out of Zn-rich solution. Magnetization, heat capacity, and resistivity measurements show that, with Al doping, the ferromagnetic phase transition temperatures of the GdFe2(AlxZn1-x) 20 compounds decrease from 86 K (x= 0) to 10 K (x= 0.122); for the nonmagnetic analog, the YFe2(AlxZn1-x) 20 series, the Stoner enhancement factor Z decreases from 0.88 (x= 0) to 0.35 (x= 0.121) in a similar manner. Tight-binding linear-muffin-tin orbital atomic-sphere approximation band structure calculations are used to rationalize this trend. These results, together with the earlier studies of the R(Fe 1-xCox)2Zn20 (R= Gd and Y) series, clearly highlight the importance of band filling and the applicability of even a simple, rigid-band model to these compounds.
UR - http://www.scopus.com/inward/record.url?scp=79961013094&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.83.054416
DO - 10.1103/PhysRevB.83.054416
M3 - Article
AN - SCOPUS:79961013094
SN - 1098-0121
VL - 83
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 5
M1 - 054416
ER -