Superconductivity under pressure in RFeAsO1−xFx (R = La, Ce−Sm) by dc magnetization measurements
Kiyotaka Miyoshi, Eiko Kojima, Saki Ogawa, Yuta Shimojo, Jun Takeuchi
DOI 10.1103/PhysRevB.87.235111 · Physical Review B
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Abstract
Superconducting transition under pressure (P) has been investigated for optimum-doped RFeAsO1−xFx (R=La, Ce–Sm) by dc magnetization measurements. For R=La, Tc is found to be pressure independent up to P∼3.0 GPa and then shows a monotonic decrease with increasing pressure. The plateau width decreases for the system with smaller lattice constants and shrinks to almost zero for R=Sm. From the Tc(P) data, we construct the Tc evolution map on the height of the As atom from the Fe-plane hAs versus lattice-constant a or c plane. It is shown that the characteristic Tc variations under pressure for all compounds and the rapid decrease in Tc induced by changing the R element from Sm to La can be described by a common Tc (hAs, a or c) surface, suggesting that Tc is determined by hAs and lattice constant. It is also suggested that there exists an upper limit of the lattice constant aulm (or culm), above which dTc/da (or dTc/dc) changes the sign from positive to negative.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| LaFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28 | Pressure unresolved | onset |
| LaFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 18 | 7 GPa | onset |
| CeFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 38 | Pressure unresolved | onset |
| CeFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 25 | 4.4 GPa | onset |
| PrFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 43 | Pressure unresolved | onset |
| PrFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 25 | 7 GPa | onset |
| NdFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 48 | 0.39 GPa | onset |
| NdFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 26 | 7.7 GPa | onset |
| SmFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 53 | Pressure unresolved | onset |
| SmFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 29 | 7.7 GPa | onset |
| LaFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 26 | Pressure not reported | unknown |
| Ba1-xKxFe2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 38 | Pressure not reported | unknown |
| Li1-xFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 18 | Pressure not reported | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8 | Pressure not reported | unknown |
| K0.8Fe2Se2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 32 | Pressure not reported | unknown |
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