TY - JOUR
T1 - Magnetic and electrical properties of NpTGa5 (T = Fe, Rh and Ni)
AU - Aoki, Dai
AU - Homma, Yoshiya
AU - Shiokawa, Yoshinobu
AU - Sakai, Hironori
AU - Yamamoto, Etsuji
AU - Nakamura, Akio
AU - Haga, Yoshinori
AU - Settai, Rikio
AU - Onuki, Yoshichika
PY - 2005/8
Y1 - 2005/8
N2 - We grew high-quality single crystals of NpTGa5 (T = Fe, Rh, and Ni) with a tetragonal structure by the Ga-flux method and measured their electrical resistivity, specific heat, magnetic susceptibility, and magnetization. All the investigated compounds undergo magnetic ordering. NpFeGa5 orders antiferromagnetically at TN = 118K and shows another magnetic transition at T* = 78 K. A relatively large electrical resistivity indicates that NpFeGa5 might be a low-carrier compound. NpRhGa5 also orders antiferromagnetically at TN1 = 36 K. Below another magnetic transition at TN2 = 32 K, the antiferromagnetic easy-axis is most likely changed from [001] to the (001) plane. On the other hand, NpNiGa5 undergoes ferromagnetic ordering at TC = 30 K, where the magnetic moment of Np is directed along the [001] direction. Furthermore, below another magnetic transition at T* = 18 K, the ordered moment is discontinuously enlarged and a change of the magnetic structure occurs. The electronic specific heat coefficients are approximately determined as 30, 52, and 100 mJ/K2·mol for NpFeGa 5, NpRhGa5, and NpNiGa5, respectively. The magnetic susceptibility approximately follows the Curie-Weiss law at high temperatures (250 < T < 300 K) with effective magnetic moments ranging from 2.4 to 2.6μB/Np for NpRhGa5 and NpNiGa 5, indicating that the localized 5f4 electronic states are most likely applicable to these compounds at high temperatures.
AB - We grew high-quality single crystals of NpTGa5 (T = Fe, Rh, and Ni) with a tetragonal structure by the Ga-flux method and measured their electrical resistivity, specific heat, magnetic susceptibility, and magnetization. All the investigated compounds undergo magnetic ordering. NpFeGa5 orders antiferromagnetically at TN = 118K and shows another magnetic transition at T* = 78 K. A relatively large electrical resistivity indicates that NpFeGa5 might be a low-carrier compound. NpRhGa5 also orders antiferromagnetically at TN1 = 36 K. Below another magnetic transition at TN2 = 32 K, the antiferromagnetic easy-axis is most likely changed from [001] to the (001) plane. On the other hand, NpNiGa5 undergoes ferromagnetic ordering at TC = 30 K, where the magnetic moment of Np is directed along the [001] direction. Furthermore, below another magnetic transition at T* = 18 K, the ordered moment is discontinuously enlarged and a change of the magnetic structure occurs. The electronic specific heat coefficients are approximately determined as 30, 52, and 100 mJ/K2·mol for NpFeGa 5, NpRhGa5, and NpNiGa5, respectively. The magnetic susceptibility approximately follows the Curie-Weiss law at high temperatures (250 < T < 300 K) with effective magnetic moments ranging from 2.4 to 2.6μB/Np for NpRhGa5 and NpNiGa 5, indicating that the localized 5f4 electronic states are most likely applicable to these compounds at high temperatures.
KW - Electrical resistivity
KW - Magnetic susceptibility
KW - Magnetization
KW - NpFeGa
KW - NpNiGa
KW - NpRhGa
KW - Specific heat
KW - Transuranium compound
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U2 - 10.1143/JPSJ.74.2323
DO - 10.1143/JPSJ.74.2323
M3 - Article
AN - SCOPUS:24644459446
SN - 0031-9015
VL - 74
SP - 2323
EP - 2331
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 8
ER -