TY - JOUR
T1 - Observation of a metamagnetic transition in the 5f heavy-fermion compound UNi2Al3
T2 - Magnetization studies up to 90 T for single-crystalline U(Pd1-xNix)2Al3 OBSERVATION of A METAMAGNETIC TRANSITION in ... KENJI MOCHIDZUKI et al.
AU - Mochidzuki, Kenji
AU - Shimizu, Yusei
AU - Kondo, Akihiro
AU - Matsuo, Akira
AU - Li, Dexin
AU - Aoki, Dai
AU - Homma, Yoshiya
AU - Honda, Fuminori
AU - Flouquet, Jacques
AU - Nakamura, Daisuke
AU - Takeyama, Shojiro
AU - Kindo, Koichi
N1 - Funding Information:
We greatly appreciate K. Suzuki's technical support in the use of the energy dispersive x-ray spectrometer at the Oarai facility at Tohoku University. We would also like to thank T. Sakakibara, A. Miyake, H. Amitsuka, N. Tateiwa, Y. Haga, A. Pourret, M. Yokoyama, Y. Matsumoto, Y. Ikeda, S. Hoshino, A. Nakamura, and A. Maurya for valuable discussions. K.M. was supported by the Japan Society for the Promotion of Science through the Program for Leading Graduate Schools (MERIT). This work is supported in part by KAKENHI (Grants No. JP15H05884, No. JP15H05882, No. JP15H05745, No. JP16H04006, No. JP17K14328). Y.S. would like to acknowledge all the support from Institute for Materials Research, Tohoku University in growing monocrystalline uranium samples using the joint research facility at Oarai.
Funding Information:
We greatly appreciate K. Suzuki's technical support in the use of the energy dispersive X-ray spectrometer at the Oarai facility at Tohoku University. We would also like to thank T. Sakakibara, A. Miyake, H. Amitsuka, N. Tateiwa, Y. Haga, A. Pourret, M. Yokoyama, Y. Matsumoto, Y. Ikeda, S. Hoshino, A. Nakamura, and A. Maurya for valuable discussions. K.M. was supported by the Japan Society for the Promotion of Science through the Program for Leading Graduate Schools (MERIT). This work is supported in part by KAKENHI (Grants No. JP15H05884, No. JP15H05882, No. JP15H05745, No. JP16H04006, No. JP17K14328). Y.S. would like to acknowledge all the support from Institute for Materials Research, Tohoku University in growing monocrystalline uranium samples using the joint research facility at Oarai..
Publisher Copyright:
© 2019 American Physical Society.
PY - 2019/10/23
Y1 - 2019/10/23
N2 - We report an observation of metamagnetism in the 5f-electron heavy-fermion antiferromagnets UNi2Al3 at 78 T and U(Pd1-xNix)2Al3 at 30 T (42 T) for x=0.5 (x=0.75) using single-crystalline samples. The magnetization curves for U(Pd1-xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic transition (MMT) field Bm, strongly indicating their first-order nature. The obtained B-T phase diagram for x=0.5 suggests the possible presence of the tricritical point, while the MMT still occurs at high temperatures above TN from paramagnetic to polarized-paramagnetic states as a crossover. The results indicate that the antiferromagnetic order is closely connected to the MMT in U(Pd1-xNix)2Al3, but the metamagnetic behavior cannot be explained by the conventional spin flip of antiferromagnetic ordered moments. Our data for U(Pd1-xNix)2Al3 have revealed an empirical linear relation of Bm(x)âTχmax(x) and a scaling behavior in magnetic susceptibility of χ(T/Tχmax)/χmax, where Tχmax is the temperature of the susceptibility maximum [χmaxχ(Tχmax)]. Importantly, the critical value of the magnetic polarization at the MMT Mcr is roughly unchanged, although the value of susceptibility is notably suppressed with increasing x.
AB - We report an observation of metamagnetism in the 5f-electron heavy-fermion antiferromagnets UNi2Al3 at 78 T and U(Pd1-xNix)2Al3 at 30 T (42 T) for x=0.5 (x=0.75) using single-crystalline samples. The magnetization curves for U(Pd1-xNix)2Al3 (x=0.5 and 0.75) show a sharp increase at the metamagnetic transition (MMT) field Bm, strongly indicating their first-order nature. The obtained B-T phase diagram for x=0.5 suggests the possible presence of the tricritical point, while the MMT still occurs at high temperatures above TN from paramagnetic to polarized-paramagnetic states as a crossover. The results indicate that the antiferromagnetic order is closely connected to the MMT in U(Pd1-xNix)2Al3, but the metamagnetic behavior cannot be explained by the conventional spin flip of antiferromagnetic ordered moments. Our data for U(Pd1-xNix)2Al3 have revealed an empirical linear relation of Bm(x)âTχmax(x) and a scaling behavior in magnetic susceptibility of χ(T/Tχmax)/χmax, where Tχmax is the temperature of the susceptibility maximum [χmaxχ(Tχmax)]. Importantly, the critical value of the magnetic polarization at the MMT Mcr is roughly unchanged, although the value of susceptibility is notably suppressed with increasing x.
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U2 - 10.1103/PhysRevB.100.165137
DO - 10.1103/PhysRevB.100.165137
M3 - Article
AN - SCOPUS:85074450721
SN - 2469-9950
VL - 100
JO - Physical Review B
JF - Physical Review B
IS - 16
M1 - 165137
ER -