Publication | Open Access
Strong-Coupling Spin-Singlet Superconductivity with Multiple Full Gaps in Hole-Doped Ba<sub>0.6</sub>K<sub>0.4</sub>Fe<sub>2</sub>As<sub>2</sub>Probed by<sup>57</sup>Fe-NMR
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References
2009
Year
Superconducting MaterialNormal StateFe-nmr MeasurementsEngineeringSpin SystemsMagnetic ResonanceSpin DynamicMagnetic MaterialsStrong-coupling Spin-singlet SuperconductivityMagnetismSuperconductivityQuantum MaterialsSuperconducting DevicesHigh-tc SuperconductivityPhysicsMultiple Full GapsCondensed Matter TheoryQuantum MagnetismKnight ShiftHigh-temperature SuperconductivityNatural SciencesCondensed Matter PhysicsApplied Physics
We present $^{57}$Fe-NMR measurements of the novel normal and superconducting-state characteristics of the iron-arsenide superconductor Ba$_{0.6}$K$_{0.4}$Fe$_2$As$_2$ ($T_c$ = 38 K). In the normal state, the measured Knight shift and nuclear spin-lattice relaxation rate $(1/T_1)$ demonstrate the development of wave-number ($q$)-dependent spin fluctuations, except at $q$ = 0, which may originate from the nesting across the disconnected Fermi surfaces. In the superconducting state, the spin component in the $^{57}$Fe-Knight shift decreases to almost zero at low temperatures, evidencing a spin-singlet superconducting state. The $^{57}$Fe-$1/T_1$ results are totally consistent with a $s^\pm$-wave model with multiple full gaps, regardless of doping with either electrons or holes.
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