TY - JOUR
T1 - Magnetic penetration depth and flux-flow resistivity measurements on NaFe0.97Co0.03As single crystals
AU - Okada, T.
AU - Takahashi, H.
AU - Imai, Y.
AU - Kitagawa, K.
AU - Matsubayashi, K.
AU - Uwatoko, Y.
AU - Maeda, A.
PY - 2013
Y1 - 2013
N2 - 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/B c2. 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) .
AB - 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/B c2. 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) .
KW - Flux-flow resistivity
KW - Iron-based superconductor
KW - Microwave surface impedance
KW - Na(Fe,Co)As
KW - Single crystal
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U2 - 10.1016/j.physc.2013.04.074
DO - 10.1016/j.physc.2013.04.074
M3 - Article
AN - SCOPUS:84884815986
SN - 0921-4534
VL - 494
SP - 109
EP - 112
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
ER -