Magnetic order and superconductivity in Y1−xPrxBa2Cu3O7
I. Felner, U. Yaron, I. Nowik, E. R. Bauminger, Y. Wolfus, E. R. Yacoby, G. Hilscher, N. Pillmayr
DOI 10.1103/PhysRevB.40.6739 · 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 system Y1−xPrxBa2Cu3−yFeyOz, with x=0 to 1, y=0 and 0.3, and z=6 and 7, has been studied by ac and dc magnetometry to determine the superconducting phase transition temperature, Tc, by Fe57 Mössbauer spectroscopy to determine the antiferromagnetic phase transition temperature of the Cu(2) site, TN, and by specific-heat measurements to determine γ and the antiferromagnetic ordering temperature of the Pr site, Tn. Tc (x,z=7), TN (x,z=6,7), and Tn (x,z=7) were obtained for x values of 0.0, 0.2, 0.4, 0.6, 0.8, and 1.0. For z=6, TN changes very little with x [TN(0,6)=415 K and TN(1,6)=350 K], but for z=7, TN changes sharply with x [TN(1,7)=325 K, TN(0.6,7)=230 K, and TN(0.4,7)≤35 K]. There is no conclusive evidence for overlap of superconductivity and antiferromagnetism. Tn also decreases strongly with decreasing x, Tn(1,7)=17 K, while Tn(0.4,7)≤2.5 K. The specific-heat measurements show large linear temperature terms. The slope γ increases strongly with x and with the introduction of the Fe probe.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| YBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 91 | Pressure not reported | unknown |
| Y0.8Pr0.2Ba2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 67 | Pressure not reported | unknown |
| Y0.6Pr0.4Ba2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 35 | Pressure not reported | unknown |
| YBa2Cu2.7Fe0.3O7.1 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 69 | Pressure not reported | unknown |
| Y0.8Pr0.2Ba2Cu2.7Fe0.3O7.1 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 25 | Pressure not reported | unknown |
Similar papers
Orthorhombic Distortion at the Superconducting Transition in YBa2Cu3O7: Evidence for Anisotropic Pairing
similarity 0.97P. M. Horn et al.
Source status unknown — claims are unverified
Magnetic order and superconductivity in RBa2Cu3Oz
similarity 0.97I. Nowik et al.
Source status unknown — claims are unverified
Magnetic properties of Y-Ba-Cu-O superconductors
similarity 0.96T. R. McGuire et al.
Source status unknown — claims are unverified
Weak-field magnetization of superconducting Y1Ba2Cu3Ox: Relationship to microstructure
similarity 0.96D. E. Farrell et al.
Source status unknown — claims are unverified
ac susceptibility near the superconducting transition in polycrystalline YBa2Cu3O7−δ
similarity 0.96W. M. Tiernan & R. B. Hallock
Source status unknown — claims are unverified
Bulk-modulus anomalies at the superconducting transition of single-phase YBa2Cu3O7
similarity 0.96D. J. Bishop et al.
Source status unknown — claims are unverified