TY - JOUR
T1 - Superconductivity and structural phase transitions in caged compounds RT2Zn20 (R=La, Pr, T = Ru, Ir)
AU - Onimaru, Takahiro
AU - Matsumoto, Keisuke T.
AU - Inoue, Yukihiro F.
AU - Umeo, Kazunori
AU - Saiga, Yuta
AU - Matsushita, Yoshitaka
AU - Tamura, Ryuji
AU - Nishimoto, Kazue
AU - Ishii, Isao
AU - Suzuki, Takashi
AU - Takabatake, Toshiro
PY - 2010/3
Y1 - 2010/3
N2 - Electrical resistivity ρ specific heat C, magnetization M measurements are reported on four compounds, LaRu2Zn20, PrRu 2Zn20, LaIr2Zn20, and PrIr2Zn20, which crystallize in a cubic CeCr2Al20- type structure. LaRu2Zn20, LaIr2Zn20, and PrIr2Zn20 show superconducting transitions at TC = 0:2, 0.6, and ∼0:05 K, respectively, whereas PrRu 2Zn20 remains a normal state down to 0.04 K. This is the first observation of superconductivity in the family of RT2X 20 (T = transition metal; X = Al and Zn). Furthermore, structural phase transitions manifest themselves at Ts = 150, 138, and 200K for LaRu2Zn20, PrRu2Zn20, and LaIr 2Zn20, respectively. No magnetic transition is found in PrRu2Zn20 and PrIr2Zn20 down to 1.8 K. On cooling PrIr2Zn20 below 2K, the specific heat divided by temperature, C=T, continuously increases and reaches 5 J/(K 2 •mol) at 0.4 K, suggesting that Pr 4f2 electrons are involved in the heavy-fermion state, as observed in a related compound YbCo2Zn20.
AB - Electrical resistivity ρ specific heat C, magnetization M measurements are reported on four compounds, LaRu2Zn20, PrRu 2Zn20, LaIr2Zn20, and PrIr2Zn20, which crystallize in a cubic CeCr2Al20- type structure. LaRu2Zn20, LaIr2Zn20, and PrIr2Zn20 show superconducting transitions at TC = 0:2, 0.6, and ∼0:05 K, respectively, whereas PrRu 2Zn20 remains a normal state down to 0.04 K. This is the first observation of superconductivity in the family of RT2X 20 (T = transition metal; X = Al and Zn). Furthermore, structural phase transitions manifest themselves at Ts = 150, 138, and 200K for LaRu2Zn20, PrRu2Zn20, and LaIr 2Zn20, respectively. No magnetic transition is found in PrRu2Zn20 and PrIr2Zn20 down to 1.8 K. On cooling PrIr2Zn20 below 2K, the specific heat divided by temperature, C=T, continuously increases and reaches 5 J/(K 2 •mol) at 0.4 K, suggesting that Pr 4f2 electrons are involved in the heavy-fermion state, as observed in a related compound YbCo2Zn20.
KW - Caged structure
KW - RTZn
KW - Structural phase transition
KW - Superconductivity
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U2 - 10.1143/JPSJ.79.033704
DO - 10.1143/JPSJ.79.033704
M3 - Article
AN - SCOPUS:77949689944
SN - 0031-9015
VL - 79
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 3
M1 - 033704
ER -