TY - JOUR
T1 - Doping evolution of the quasiparticle excitations in heavily hole-doped Ba 1 - X K x Fe 2 As 2
T2 - A possible superconducting gap with sign-reversal between hole pockets
AU - Watanabe, D.
AU - Yamashita, T.
AU - Kawamoto, Y.
AU - Kurata, S.
AU - Mizukami, Y.
AU - Ohta, T.
AU - Kasahara, S.
AU - Yamashita, M.
AU - Saito, T.
AU - Fukazawa, H.
AU - Kohori, Y.
AU - Ishida, S.
AU - Kihou, K.
AU - Lee, C. H.
AU - Iyo, A.
AU - Eisaki, H.
AU - Vorontsov, A. B.
AU - Shibauchi, T.
AU - Matsuda, Y.
PY - 2014/3/11
Y1 - 2014/3/11
N2 - To gain insight into the unconventional superconductivity of Fe pnictides with no electron pockets, we measure the thermal conductivity κ and penetration depth λ in the heavily hole-doped regime of Ba1-xKxFe2As2. The residual thermal conductivity (κ/T)T→0K and T dependence of λ consistently indicate the fully gapped superconductivity at x=0.76 and the (line) nodal superconductivity at higher hole concentrations. The magnitude of κTTc|T→0K and the slope of λ(T) at low temperatures, both of which are determined by the properties of the low-energy excitations, exhibit a highly unusual nonmonotonic x dependence. These results indicate a dramatic change of the nodal characteristics in a narrow doping range. We suggest that the observed x dependence is naturally explained by a doping crossover of the gap function between the s-wave states with and without sign reversal between Γ-centered hole pockets.
AB - To gain insight into the unconventional superconductivity of Fe pnictides with no electron pockets, we measure the thermal conductivity κ and penetration depth λ in the heavily hole-doped regime of Ba1-xKxFe2As2. The residual thermal conductivity (κ/T)T→0K and T dependence of λ consistently indicate the fully gapped superconductivity at x=0.76 and the (line) nodal superconductivity at higher hole concentrations. The magnitude of κTTc|T→0K and the slope of λ(T) at low temperatures, both of which are determined by the properties of the low-energy excitations, exhibit a highly unusual nonmonotonic x dependence. These results indicate a dramatic change of the nodal characteristics in a narrow doping range. We suggest that the observed x dependence is naturally explained by a doping crossover of the gap function between the s-wave states with and without sign reversal between Γ-centered hole pockets.
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U2 - 10.1103/PhysRevB.89.115112
DO - 10.1103/PhysRevB.89.115112
M3 - Article
AN - SCOPUS:84897009671
SN - 1098-0121
VL - 89
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 11
M1 - 115112
ER -