Abstract

We measured the surface impedance of NaFe1−xCoxAs (x≈0.03, optimally doped) single crystals under finite magnetic fields. At low temperatures (T<0.5Tc), the penetration depth of these crystals was increased as λ(T)−λ(0)=A×Tn with an exponent n≈2, indicating the realization of the gapless superconductivity. The flux-flow resistivity, ρf, behaved similarly to the Bardeen–Stephen prediction, ρf/ρn=B/Bc2. However, the electronic state inside the vortex core was not so dirty. By comparing the results with those of LiFeAs1−xPx and SrFe2(As0.7P0.3)2, it has been clarified that the gap anisotropy dominates the gradient of ρf(B).

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