← Back to search

Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+δ by controlling disorder outside CuO2 planes

H. Hobou, S. Ishida, K. Fujita, M. Ishikado, K. M. Kojima, H. Eisaki, S. Uchida

DOI 10.1103/PhysRevB.79.064507 · Physical Review B

T1

Active bibliographic source — not scientific approval

Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.

Abstract

We investigate the effect of disorder at various lattice sites outside the CuO2 plane on the superconducting critical temperature Tc of the cuprate superconductor Bi2Sr2CaCu2O8+δ (Bi2212). The most effective disorder turns out to be that at the Sr site in the neighboring blocks, which contain apical-oxygen atoms. The Sr-site disorder reduces Tc and also produces a residual component (ρ0) in the in-plane resistivity, the magnitude of which is found to be proportional to the magnitude of Tc reduction. We demonstrate that both the Tc-degradation rate and ρ0 decrease as the number of the CuO2 planes increases in the unit cell, that is, as the number of the neighboring SrO blocks decreases. In real crystals of Bi-based cuprates, main source of disorder is Bi atoms randomly occupying the Sr sites. We have succeeded in reducing the Bi content at Sr sites as much as possible and achieved Tc=98 K, a high-Tc record in Bi2212.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Bi2Sr2CaCu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

92Pressure not reportedonset
Bi2.02Sr1.98Ca0.85Y0.08Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

96Pressure not reportedonset
Bi1.69Pb0.33Sr1.96Ca0.92Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

96Pressure not reportedonset
Bi1.42Pb0.55Sr1.97Ca0.96Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

97.5Pressure not reportedonset
Bi1.31Pb0.66Sr1.94Ca1.08Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

94Pressure not reportedonset
Bi1.58Pb0.36Sr1.92Ca0.93Y0.11Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

94Pressure not reportedonset
Bi1.50Pb0.37Sr1.97Ca0.92Y0.05Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

96Pressure not reportedonset
Bi1.33Pb0.65Sr2.00Ca0.98Y0.03Cu2O8+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

98Pressure not reportedonset
Sr2CuO3+δ

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

95Pressure not reportedunknown

Similar papers