Synthesis, structural, and transport properties of the hole-doped superconductor Pr1−xSrxFeAsO
Gang Mu, Bin Zeng, Xiyu Zhu, Fei Han, Peng Cheng, Bing Shen, Hai-Hu Wen
DOI 10.1103/PhysRevB.79.104501 · Physical Review B
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Abstract
Superconductivity was achieved in PrFeAsO by partially substituting Pr3+ with Sr2+. The electrical transport properties and structure of this superconductor Pr1−xSrxFeAsO at different doping levels (x=0.05∼0.25) were investigated systematically. It was found that the lattice constants (a and c axes) increase monotonously with Sr or hole concentration. The superconducting transition temperature at about 16.3 K (95% ρn) was observed around the doping level of 0.20∼0.25. A detailed investigation was carried out in the sample with doping level of x=0.25. The domination of holelike charge carriers in this material was confirmed by Hall-effect measurements. The magnetoresistance (MR) behavior can be well described by a simple two-band model. The upper critical field of the sample with Tc=16.3 K (x=0.25) was estimated to be beyond 45 T. Our results suggest that the hole-doped samples may have higher upper critical fields comparing to the electron-doped ones, due to the higher quasiparticle density of states at the Fermi level.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Pr1-xSrxFeAsO Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 16.3 | Pressure not reported | onset |
| Pr0.75Sr0.25FeAsO Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 16.3 | Pressure not reported | onset |
| Pr0.75Sr0.25FeAsO Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 16.3 | Pressure not reported | zero_resistance |
| 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 |
| La1-xSrxFeAsO Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 25 | Pressure not reported | unknown |
| Nd1-xSrxFeAsO Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 13.5 | Pressure not reported | unknown |
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