TY - JOUR
T1 - Phase diagram and transport properties of Y1-xNdxCo2 pseudo-binary alloys
AU - Burkov, A. T.
AU - Takeda, M.
AU - Teruya, A.
AU - Watanabe, S.
AU - Hirakawa, S.
AU - Hiranaka, Y.
AU - Nakamura, A.
AU - Hedo, M.
AU - Nakama, T.
AU - Yagasaki, K.
AU - Takaesu, Y.
AU - Uchima, K.
AU - Uwatoko, Y.
N1 - Funding Information:
Part of this work was supported by a Grant-in-Aid for Scientific Research (No. 21540340) from the Ministry of Education, Culture, Sports, Science and Technology of Japan and by Russian Foundation for Basic Research under the Grant 09-02-01285a.
PY - 2013/7
Y1 - 2013/7
N2 - The electrical resistivity ρ and the thermopower S of pseudo-binary Y1-xNdxCo2 alloys have been measured at temperatures from 2 to 300 K under pressures up to 3.5 GPa. NdCo2 is a ferromagnet with a Curie temperature T C of 98 K. In the ferromagnetic phase, it undergoes a 4f spin-reorientation transition at T R = 40 K. At this transition, the easy direction of 4f magnetization is changed from [100] at temperatures above T R to [110] below T R. The system phase diagram T C(x, P) and T R(x, P) is inferred from the temperature dependencies of the electrical resistivity and the thermopower. The Curie temperature of the alloys, TC decreases with decreasing Nd concentration x and vanishes around x c = 0.3. Above x c, the Curie temperature decreases with increasing pressure. The spinreorientation temperature weakly depends on the composition and on the pressure until it merges with T C. There is a large region of the phase diagram, partly overlapping with the ferromagnetic phase, where the cobalt 3d electron system is non-uniformly magnetized due to spatial fluctuations of the 4f-3d exchange field related to a random distribution of Nd 4f magnetic moments over the R sublattice. In this region, large static 3d magnetic fluctuations govern the electronic transport.
AB - The electrical resistivity ρ and the thermopower S of pseudo-binary Y1-xNdxCo2 alloys have been measured at temperatures from 2 to 300 K under pressures up to 3.5 GPa. NdCo2 is a ferromagnet with a Curie temperature T C of 98 K. In the ferromagnetic phase, it undergoes a 4f spin-reorientation transition at T R = 40 K. At this transition, the easy direction of 4f magnetization is changed from [100] at temperatures above T R to [110] below T R. The system phase diagram T C(x, P) and T R(x, P) is inferred from the temperature dependencies of the electrical resistivity and the thermopower. The Curie temperature of the alloys, TC decreases with decreasing Nd concentration x and vanishes around x c = 0.3. Above x c, the Curie temperature decreases with increasing pressure. The spinreorientation temperature weakly depends on the composition and on the pressure until it merges with T C. There is a large region of the phase diagram, partly overlapping with the ferromagnetic phase, where the cobalt 3d electron system is non-uniformly magnetized due to spatial fluctuations of the 4f-3d exchange field related to a random distribution of Nd 4f magnetic moments over the R sublattice. In this region, large static 3d magnetic fluctuations govern the electronic transport.
KW - Electrical resistivity
KW - Pressure effect
KW - Thermopower
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U2 - 10.3938/jkps.62.2080
DO - 10.3938/jkps.62.2080
M3 - Article
AN - SCOPUS:84880014640
SN - 0374-4884
VL - 62
SP - 2080
EP - 2083
JO - Journal of the Korean Physical Society
JF - Journal of the Korean Physical Society
IS - 12
ER -