Specific-heat anomaly near Tc of the (Bi,Pb)-Sr-Ca-Cu-O superconductor (Tc=107 K)
N. Okazaki, T. Hasegawa, K. Kishio, K. Kitazawa, A. Kishi, Y. Ikeda, M. Takano, K. Oda, H. Kitaguchi, J. Takada, Y. Miura
DOI 10.1103/PhysRevB.41.4296 · Physical Review B
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Abstract
Specific-heat measurements of the 107-K phase of the (Bi,Pb)-Sr-Ca-Cu-O system were made in the temperature range 80–250 K by an ac calorimetry method. A finite specific-heat jump at Tc (ΔCp/Tc=16 mJ mol−1 K−2) was first detected, from which the electronic specific-heat coefficient was calculated through the BCS relationship, i.e., 11 mJ mol−1 K−2, corresponding to the density of states N(0)=0.8 states eV−1 (Cu atom)−1 spin−1. This N(0) value was rather smaller than that of (La1−xMx)2CuO4 (M=1/rSr,Ca) or Ba2YCu3O7. This is in contrast with the usually observed positive correlation between Tc and N(0) among the conventional metallic superconductors. A broadened transition width and the sharpened peak at Tc observed in the Cp–T curve was attributed to the two-dimensional superconducting fluctuation effect with coherence length ξ(0)=13 i/rÅ in the plane.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| (Bi,Pb)-Sr-Ca-Cu-O Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 107 | Pressure not reported | onset |
| (Bi,Pb)-Sr-Ca-Cu-O Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 108 | Pressure not reported | midpoint |
| Ba2YCu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Bi2Sr2CaCu2O8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 80 | Pressure not reported | unknown |
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