Superconductivity and antiferromagnetism in La2−xCa1+xCu2O6±δ and La2−xSrxCaCu2O6±δ
K. Kinoshita, T. Yamada
DOI 10.1103/PhysRevB.46.9116 · Physical Review B
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
La2CaCu2O6 can be made superconducting by doping Ca or Sr in the form of La2−x(Sr,Ca)xCaCu2O6+δ and by synthesis under high O2 pressures of more than 4 atm. Superconducting properties of La2−xCa1+xCu2O6±δ (0.08≤x≤0.25) and La2−xSrxCaCu2O6±δ (0.07≤x≤0.23) as functions of composition (x) and oxygen partial pressure during synthesis (PO2 up to 400 atm) were investigated by measuring their electrical resistivity and magnetic susceptibility. In both compounds, the superconducting transition temperature (Tc) increased with increasing x and PO2, and showed almost the same maximum Tc (zero) of about 51 K at the solubility limit of Ca or Sr in La (x≊0.25) with PO2 at 400 atm, although at a lower PO2, Tc (zero) was higher in a Sr-doped compound than that of a Ca- doped compound. Nonsuperconducting or weakly superconducting La2−xCa1+xCu2O6±δ and La2−xSrxCaCu2O6±δ synthesized under oxygen partial pressures between 0.2 and 10 atm showed cusps in their magnetic susceptibility at around 25 K, which may result from three-dimensional (3D) antiferromagnetic ordering. The superconductivity of these compounds may appear as a result of the frustration of such 3D antiferromagnetic correlation as with other copper oxide superconductors.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| La1.82Ca1.18Cu2O6±δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 49 | Pressure not reported | zero_resistance |
| La1.82Ca1.18Cu2O6±δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 60 | Pressure not reported | onset |
| La2-xCa1+xCu2O6±δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 51 | Pressure not reported | zero_resistance |
| La2-xSrxCaCu2O6±δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 51 | Pressure not reported | zero_resistance |
| La1.6Sr0.4CaCu2O6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La1.85(Ca0.86Sr0.14)1.15Cu2O6.03 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Superconducting-plasma resonance along the c axis in various copper oxide superconductors
similarity 0.96H. Shibata & T. Yamada
Source status unknown — claims are unverified
Antiferromagnetic order and high-temperature superconductivity
similarity 0.96Kerson Huang & Efstratios Manousakis
Source status unknown — claims are unverified
Total Suppression of Superconductivity by High Magnetic Fields in YBa2Cu3O6.6
similarity 0.95F. Rullier-Albenque et al.
Source status unknown — claims are unverified
Evidence for antiferromagnetic interactions in the high-temperature superconductor La1.85Sr0.15CuO4−y
similarity 0.95P. Gutsmiedl et al.
Source status unknown — claims are unverified
Interlayer coupling and the thermopower of cuprate superconductors
similarity 0.95J.-S. Zhou & J. B. Goodenough
Source status unknown — claims are unverified
Anomalous properties and microstructural model of superconductivity in La2−x(Ba,Sr)xCuO4
similarity 0.95J. C. Phillips & Karin M. Rabe
Source status unknown — claims are unverified