Stabilization of the tetragonal phase and superconducting behavior in RBa2(Cu1−xFex)3Oy (R=Y,Gd; 0≤x≤0.15)
T. J. Kistenmacher, W. A. Bryden, J. S. Morgan, K. Moorjani, Y- W. Du, Z. Q. Qiu, H. Tang, J. C. Walker
DOI 10.1103/PhysRevB.36.8877 · 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
The structure and superconductivity for YBa2(Cu1−xFex)3Oy and GdBa2(Cu1−xFex)3Oy ceramics (0≤x≤0.15) have been studied by x-ray diffraction and resistivity measurements. In each family of materials (but more rapidly in the Gd ceramics), increasing Fe substitution leads to the stabilization of the tetragonal perovskite structure and suppression of superconductivity, apparently owing to pair breaking by the Fe moments. Anomalous behavior at higher Fe substitution is attributed to the combined influence of Gd and Fe moments.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YBa2Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 95 | Pressure not reported | unknown |
| YBa2(Cu1-xFex)3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 93.5 | Pressure not reported | unknown |
| GdBa2(Cu1-xFex)3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 93.5 | Pressure not reported | unknown |
| YBa2(Cu0.88Fe0.12)3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 37 | Pressure not reported | unknown |
| YBa2(Cu0.85Fe0.15)3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 15 | Pressure not reported | onset |
Similar papers
Microstructure, lattice parameters, and superconductivity of YBa2(Cu1−xFex)3O7−δ for 0≤x≤0.33
similarity 0.96Youwen Xu et al.
Source status unknown — claims are unverified
High-pressure oxidation of the tetragonal La1.5−xBa1.5+x−yCayCu3Oz superconductors
similarity 0.96J. M. S. Skakle et al.
Source status unknown — claims are unverified
Role of Ba-site Pr in quenching superconductivity of Y1−yPryBa2Cu3Ox and related materials
similarity 0.95Howard A. Blackstead & John D. Dow
Source status unknown — claims are unverified
Effect of compositional variation and annealing in oxygen on superconducting properties of Y1Ba2Cu3O8−y
similarity 0.95A. J. Panson et al.
Source status unknown — claims are unverified
Possibility of high-temperature superconductivity in an ordered tetragonal crystal structure in RBa2Cu3O7 (R= rare earth) superconductors
similarity 0.95Raju P. Gupta & Michèle Gupta
Source status unknown — claims are unverified
Metallization and superconducting properties of YBa2Cu3O6.2Bry
similarity 0.95H. B. Radousky et al.
Source status unknown — claims are unverified