Anisotropic resistivity of NaFeCoAs
arXiv:1208.3646 · doi:10.1103/PhysRevB.86.144528
Abstract
Temperature-dependent resistivity is studied in single crystals of iron-arsenide superconductor NaFeCoAs for electrical current directions along, , and transverse, , to the Fe-As layers. Doping with Co increases stability of this compound to reaction with the environment and suppresses numerous features in both and compared to the stoichiometric NaFeAs. Evolution of with follows a universal trend observed in other pnictide superconductors, exhibiting a -linear temperature dependence close to the optimal doping and development of dependence upon further doping. in parent compound shows a non - monotonic behavior with a crossover from non-metallic resistivity increase on cooling from room temperature down to 80 K to a metallic decrease below this temperature. Both and show several correlated crossover - like features at 80 K. Despite a general trend towards more metallic behavior of inter - plane resistivity in Co-doped samples, the temperature of the crossover from insulating to metallic behavior (80 K) does not change much with doping.
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Cited by in corpus (16)
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- The upper critical field of NaFeCoAs superconductors
- Temperature-concentration phase diagram of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors
- Interplane resistivity of underdoped single crystals (BaK)FeAs,
- Inter-plane resistivity of isovalent doped BaFe(AsP)
- Crystal growth and the electronic phase diagram of the 4 doped NaFeRhAs in comparison with 3 doped NaFeCoAs
- Electron doping evolution of the magnetic excitations in NaFeCoAs
- Electron doping evolution of the neutron spin resonance in NaFeCoAs
- Phase diagram and neutron spin resonance of superconducting NaFeCuAs
- Local Structure and Hyperfine Interactions of 57Fe in NaFeAs Studied by Mossbauer Spectroscopy
- Superconductivity-induced Phonon Renormalization on NaFeCoAs
- Temperature and polarization dependence of low-energy magnetic fluctuations in nearly-optimal-doped NaFeCoAs
- Combined resistivity and Hall effect study on NaFeRhAs single crystals