Evolution of normal and superconducting properties of single crystals of Na1–δFeAs upon interaction with environment
M. A. Tanatar, N. Spyrison, Kyuil Cho, E. C. Blomberg, Guotai Tan, Pengcheng Dai, Chenglin Zhang, R. Prozorov
DOI 10.1103/PhysRevB.85.014510 · Physical Review B
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Abstract
Iron-arsenide superconductor Na1–δFeAs is highly reactive with the environment. Due to the high mobility of Na ions, this reaction affects the entire bulk of the crystals and leads to an effective stoichiometry change. Here we use this effect to study the doping evolution of normal and superconducting properties of the same single crystals. Controlled reaction with air increases the superconducting transition temperature Tc from the initial value of 12 to 27 K as probed by transport and magnetic measurements. Similar effects are observed in samples reacted with Apiezon N grease, which slows down the reaction rate and results in more homogeneous samples. In both cases, the temperature-dependent resistivity ρa(T) shows a dramatic change with exposure time. In freshly prepared samples, ρa(T) reveals clear features at the tetragonal-to-orthorhombic (Ts≈60 K) and antiferromagnetic (Tm=45 K) transitions and superconductivity with onset Tc,ons=16 K and offset Tc,off=12 K. The exposed samples show T-linear variation of ρa(T) above Tc,ons=30 K (Tc,off=26 K), suggesting bulk character of the observed doping evolution and implying the existence of a quantum critical point at the optimal doping. The resistivity for different doping levels is affected below ∼200 K suggesting the existence of a characteristic energy scale that terminates the T-linear regime, which could be identified with a pseudogap.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Na1-δFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12 | Pressure not reported | unknown |
| NaFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 13 | Pressure not reported | onset |
| NaFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 24 | Pressure not reported | onset |
| NaFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 28 | Pressure not reported | onset |
| Na1-δFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 14 | Pressure not reported | onset |
| Na1-δFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12 | Pressure not reported | zero_resistance |
| Na1-δFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| Na1-δFeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 26 | Pressure not reported | zero_resistance |
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