← Back to search

Sr3Sc2Fe2As2O5 as a possible parent compound for FeAs-based superconductors

Xiyu Zhu, Fei Han, Gang Mu, Bin Zeng, Peng Cheng, Bing Shen, Hai-Hu Wen

DOI 10.1103/PhysRevB.79.024516 · Physical Review B

T1

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

A compound with the FeAs-layers, namely, (Sr3Sc2O5)Fe2As2 (abbreviated as FeAs-32522), was successfully fabricated. It has a layered structure with the space group of I4/mmm, and with the lattice constants a=4.069 Å and c=26.876 Å. The in-plane Fe ions construct a square lattice which is close to that of other FeAs-based superconductors, such as REFeAsO (RE=rare earth elements) and (Ba,Sr)Fe2As2. However the inter-FeAs-layer spacing in the compound is greatly enlarged. The temperature dependence of resistivity exhibits a weak upturn in the low-temperature region, but a metallic behavior was observed above about 60 K. The magnetic susceptibility shows also a nonmonotonic behavior. Interestingly, the well-known resistivity anomaly which was discovered in all other parent compounds, such as REFeAsO, (Ba,Sr)Fe2As2 and (Sr,Ca,Eu)FeAsF and associated with the spin-density wave/structural transition has not been found in the new system either on the resistivity data or the magnetization data. This could be induced by the large spacing distance between the FeAs-planes, therefore the antiferromagnetic correlation between the moments of Fe ions in neighboring FeAs layers cannot be established. Alternatively it can also be attributed to the self-doping effect between Fe and Sc ions. The Hall coefficient RH is negative but strongly temperature dependent in wide temperature region, which indicates the dominance of electrical conduction by electronlike charge carriers and probably a multiband effect or a spin related scattering effect. It is found that the magnetoresistance cannot be described by Kohler’s rule, which gives further support to above arguments.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
SmFeAsO

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

55Pressure not reportedunknown
LixFeAs

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

18Pressure not reportedunknown
FeSe1-x

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

8Pressure not reportedunknown
La3Ni4O2P4

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

2.2Pressure not reportedunknown
La1-xSrxCuO4

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

38Pressure not reportedunknown
Bi2Sr2CuO6

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

38Pressure not reportedunknown
YBa2Cu3O7

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

92Pressure not reportedunknown
Bi2Sr2CaCu2O8

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

92Pressure not reportedunknown
Bi2Sr2Ca2Cu3O10

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

123Pressure unresolvedunknown

Similar papers