TY - JOUR
T1 - Pressure-temperature-field phase diagram in the ferromagnet U3P4
AU - Araki, Shingo
AU - Hayashida, Minami
AU - Nishiumi, Naoto
AU - Manabe, Hiroki
AU - Ikeda, Yoichi
AU - Kobayashi, Tatsuo C.
AU - Murata, Keizo
AU - Inada, Yoshihiko
AU - Wis̈niewski, Piotr
AU - Aoki, Dai
AU - Onuki, Yoshichika
AU - Yamamoto, Etsuji
AU - Haga, Yoshinori
N1 - Publisher Copyright:
© 2015 The Physical Society of Japan.
PY - 2015/2/15
Y1 - 2015/2/15
N2 - The pressure-temperature-field phase diagram and quantum fluctuation effect were investigated in the itinerant ferromagnet U3P4 by resistivity, ac susceptibility, and Hall effect measurements under high pressure. The zerotemperature ferromagnetic-to-paramagnetic transition is located at Pc ∼ 4.0 GPa. The tricritical point exists at P∗ = 3.8 GPa and T∗ = 32K, where the ferromagnetic transition changes from second- to first-order. As a quantum fluctuation effect, the low-temperature resistivity at Pc follows T5/3 dependence, which was theoretically described in the case of a three-dimensional ferromagnet. This result indicates that the ferromagnetic-to-paramagnetic transition at Pc may be considered as weakly first-order. Another critical behavior, the huge enhancement of ρ0 observed at Pc, cannot be interpreted as the ferromagnetic fluctuation effect. The Hall effect measurements suggest that the magnetic structure in the ordered state changes under high pressure.
AB - The pressure-temperature-field phase diagram and quantum fluctuation effect were investigated in the itinerant ferromagnet U3P4 by resistivity, ac susceptibility, and Hall effect measurements under high pressure. The zerotemperature ferromagnetic-to-paramagnetic transition is located at Pc ∼ 4.0 GPa. The tricritical point exists at P∗ = 3.8 GPa and T∗ = 32K, where the ferromagnetic transition changes from second- to first-order. As a quantum fluctuation effect, the low-temperature resistivity at Pc follows T5/3 dependence, which was theoretically described in the case of a three-dimensional ferromagnet. This result indicates that the ferromagnetic-to-paramagnetic transition at Pc may be considered as weakly first-order. Another critical behavior, the huge enhancement of ρ0 observed at Pc, cannot be interpreted as the ferromagnetic fluctuation effect. The Hall effect measurements suggest that the magnetic structure in the ordered state changes under high pressure.
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U2 - 10.7566/JPSJ.84.024705
DO - 10.7566/JPSJ.84.024705
M3 - Article
AN - SCOPUS:84925002500
SN - 0031-9015
VL - 84
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 2
M1 - 024705
ER -