TY - JOUR
T1 - Superconducting and fermi surface properties of pyrite-type compounds CuS2 and CuSe2
AU - Kakihana, Masashi
AU - Matsuda, Tatsuma D.
AU - Higashinaka, Ryuji
AU - Aoki, Yuji
AU - Nakamura, Ai
AU - Aoki, Dai
AU - Harima, Hisatomo
AU - Hedo, Masato
AU - Nakama, Takao
AU - Ōnuki, Yoshichika
N1 - Funding Information:
This work was supported by JSPS KAKENHI Grant Numbers JP18J15180, JP18H04329, JP17K05547, JP16K05453, JP16K05454, JP16H04006, JP15H05886, and JP15H05884.
PY - 2019
Y1 - 2019
N2 - We grew high-quality single crystals of the pyrite-type compounds CuS2 and CuSe2 under a pressure of 5 GPa and studied their superconducting and Fermi surface properties by measuring their electrical resistivity, specific heat, and de Haas–van Alphen (dHvA) effect. The upper critical field Hc2 at 0 K [Hc2(0)] is found to be small, Hc2(0) = 160 Oe in CuS2 with the superconducting transition temperature Tsc of 1.5 K and Hc2(0) = 610 Oe in CuSe2 with Tsc of 2.4 K. The detected dHvA branches are small in number in CuS2, but the main dHvA branches, which are expected to exist in the energy band calculations, are hardly observed in CuSe2. The cyclotron effective masses are not large, ranging from 0.8 to 2.4 m0, revealing that the correlation between Cu-3d conduction electrons is weaker than those of the other pyrite-type compounds of the ferromagnet CoS2 and the Mott–Hubbard insulator NiS2.
AB - We grew high-quality single crystals of the pyrite-type compounds CuS2 and CuSe2 under a pressure of 5 GPa and studied their superconducting and Fermi surface properties by measuring their electrical resistivity, specific heat, and de Haas–van Alphen (dHvA) effect. The upper critical field Hc2 at 0 K [Hc2(0)] is found to be small, Hc2(0) = 160 Oe in CuS2 with the superconducting transition temperature Tsc of 1.5 K and Hc2(0) = 610 Oe in CuSe2 with Tsc of 2.4 K. The detected dHvA branches are small in number in CuS2, but the main dHvA branches, which are expected to exist in the energy band calculations, are hardly observed in CuSe2. The cyclotron effective masses are not large, ranging from 0.8 to 2.4 m0, revealing that the correlation between Cu-3d conduction electrons is weaker than those of the other pyrite-type compounds of the ferromagnet CoS2 and the Mott–Hubbard insulator NiS2.
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U2 - 10.7566/JPSJ.88.014702
DO - 10.7566/JPSJ.88.014702
M3 - Article
AN - SCOPUS:85058973112
SN - 0031-9015
VL - 88
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 1
M1 - 014702
ER -