TY - JOUR
T1 - Superconductivity of (Hg0.7Tl0.3)2Ba2Y 1-xCaxCu2O8-δ (0 ≦ x ≦ 0.8) with a wide range of doping state
AU - Tokiwa-Yamamoto, Ayako
AU - Tatsuki, Tadashi
AU - Adachi, Seiji
AU - Tanabe, Keiichi
N1 - Funding Information:
This work was supported by NEDO for the R&D of Industrial Science and Technology Frontier Program.
PY - 1996/9/10
Y1 - 1996/9/10
N2 - (Hg,Tl)-based cuprates with the nominal compositions of (Hg0.7Tl0.3)2Ba2Y 1-xCaxCu2O8-δ (0 ≦ x ≦ 1.0, every 0.1 step) were prepared under high pressure, and nearly single phases were obtained for the samples with 0 ≦ x ≦ 0.8. We systematically investigated their unit cell dimensions, DC susceptibility, electrical resistivity, oxygen content and copper valence as a function of Ca content, x. For the samples with x = 0-0.4, Tc, which was determined by DC susceptibility, increased from 12 K to 84 K with increasing x, while the samples with x = 0.5-0.8 exhibited a Tc decrease from 84 K to 40 K. This result indicates that the doping state of the samples can be extensively varied from underdoped to overdoped states by the Ca substitution. This variation in the doping states was also supported by the systematic change in the temperature dependence of the electrical resistivity. Oxygen analysis revealed that the copper valence gradually increased from 2.12 to 2.26 with increasing x from 0 to 0.8. The copper valence with the maximum Tc of 84 K in these samples was determined to be 2.18-2.19, which is comparable to the value for the optimum Tc in other high-Tc cuprates.
AB - (Hg,Tl)-based cuprates with the nominal compositions of (Hg0.7Tl0.3)2Ba2Y 1-xCaxCu2O8-δ (0 ≦ x ≦ 1.0, every 0.1 step) were prepared under high pressure, and nearly single phases were obtained for the samples with 0 ≦ x ≦ 0.8. We systematically investigated their unit cell dimensions, DC susceptibility, electrical resistivity, oxygen content and copper valence as a function of Ca content, x. For the samples with x = 0-0.4, Tc, which was determined by DC susceptibility, increased from 12 K to 84 K with increasing x, while the samples with x = 0.5-0.8 exhibited a Tc decrease from 84 K to 40 K. This result indicates that the doping state of the samples can be extensively varied from underdoped to overdoped states by the Ca substitution. This variation in the doping states was also supported by the systematic change in the temperature dependence of the electrical resistivity. Oxygen analysis revealed that the copper valence gradually increased from 2.12 to 2.26 with increasing x from 0 to 0.8. The copper valence with the maximum Tc of 84 K in these samples was determined to be 2.18-2.19, which is comparable to the value for the optimum Tc in other high-Tc cuprates.
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U2 - 10.1016/0921-4534(96)00414-5
DO - 10.1016/0921-4534(96)00414-5
M3 - Article
AN - SCOPUS:0030246784
SN - 0921-4534
VL - 268
SP - 191
EP - 196
JO - Physica C: Superconductivity and its applications
JF - Physica C: Superconductivity and its applications
IS - 3-4
ER -