Upper critical field and quantum oscillations in tetragonal superconducting FeS

被引:14
作者
Terashima, Taichi [1 ]
Kikugawa, Naoki [1 ]
Lin, Hai [2 ,3 ]
Zhu, Xiyu [2 ,3 ]
Wen, Hai-Hu [2 ,3 ]
Nomoto, Takuya [4 ]
Suzuki, Katsuhiro [5 ]
Ikeda, Hiroaki [6 ]
Uji, Shinya [1 ]
机构
[1] Natl Inst Mat Sci, Tsukuba, Ibaraki 3050003, Japan
[2] Nanjing Univ, Ctr Superconducting Phys & Mat, Natl Lab Solid State Microstruct, Nanjing 210093, Jiangsu, Peoples R China
[3] Nanjing Univ, Dept Phys, Natl Ctr Microstruct & Quantum Manipulat, Nanjing 210093, Jiangsu, Peoples R China
[4] Kyoto Univ, Dept Phys, Kyoto 6068502, Japan
[5] Ritsumeikan Univ, Res Org Sci & Technol, Kusatsu, Shiga 5258577, Japan
[6] Ritsumeikan Univ, Dept Phys, Kusatsu, Shiga 5258577, Japan
基金
中国国家自然科学基金;
关键词
PHASE;
D O I
10.1103/PhysRevB.94.100503
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The magnetoresistance and magnetic torque of FeS are measured in magnetic fields B of up to 18 T down to a temperature of 0.03 K. The superconducting transition temperature is found to be T-c = 4.1 K, and the anisotropy ratio of the upper critical field B-c2 at Tc is estimated from the initial slopes to be Gamma (T-c) = 6.9. B-c2(0) is estimated to be 2.2 and 0.36 T for B parallel to ab and c, respectively. Quantum oscillations are observed in both the resistance and torque. Two frequencies F = 0.15 and 0.20 kT are resolved and assigned to a quasi-two-dimensional Fermi surface cylinder. The carrier density and Sommerfeld coefficient associated with this cylinder are estimated to be 5.8 x 10(-3) carriers/Fe and 0.48 mJ/(K-2 mol), respectively. Other Fermi surface pockets still remain to be found. Band-structure calculations are performed and compared to the experimental results.
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页数:6
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