Long-range magnetic ordering in the high-Tc superconductors RBa2Cu3O7−δ (R=Nd, Sm, Gd, Dy, and Er)
B. W. Lee, J. M. Ferreira, Y. Dalichaouch, M. S. Torikachvili, K. N. Yang, M. B. Maple
DOI 10.1103/PhysRevB.37.2368 · Physical Review B
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Abstract
Low-teperature specific-heat C measurements have been made on the high-Tc superconductors RBa2Cu3O7−δ (R=Nd, Sm, Gd, Dy, and Er; δ≊0.1) for 0.5≲T≤30 K. Features in the specific heat associated with magnetic ordering of the trivalent R ions were observed for all of these compounds. The values of the magnetic ordering temperature TM, defined as the temperature of the peak of the specific-heat anomaly due to magnetic ordering, are 0.52, 0.61, 2.25, 0.90, and 0.60 K for the compounds with R=Nd, Sm, Gd, Dy, and Er, respectively. Calculations of the magnetic entropy from the C vs T data suggest that the R ions in these compounds have doublet ground states, except for R=Gd, which has an eightfold degenerate ground state. The values of TM for the compounds with R=Nd, Sm, Dy, and Er are in reasonable agreement with the deGennes factor scaling of TM for the compound with R=Gd. The deGennes factor scaling of TM is consistent with expectations based on the Ruderman-Kittel-Kasuya-Yosida interaction, although the agreement may be fortuitous since recent specific-heat measurements by Dunlap et al. on metallic and semiconducting (oxygen-defiicient) GdBa2Cu3O7−δ suggest that dipole-dipole interactions are responsible for the magnetic order in these materials.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| NdBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | onset |
| SmBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | onset |
| GdBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | onset |
| DyBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | onset |
| ErBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | onset |
| YBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90 | Pressure not reported | unknown |
| LaBa2Cu3O7-δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 56 | Pressure not reported | unknown |
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