Abstract

The in-plane London penetration depth, λ(T)λ(T), was measured in single crystals of the iron-chalcogenide superconductors Fe1.03_{1.03}(Te0.63_{0.63}Se0.37_{0.37}) and Fe1.06_{1.06}(Te0.88_{0.88}S0.14_{0.14}) by using a radio-frequency tunnel diode resonator. As is also the case for the iron-pnictides, these iron-chalcogenides exhibit a nearly quadratic temperature variation of λ(T)λ(T) at low temperatures. The absolute value of the penetration depth in the T→0T \to 0 limit was determined for Fe1.03_{1.03}(Te0.63_{0.63}Se0.37)_{0.37}) by using an Al coating technique, giving λ(0)≈560±20λ(0)\approx560 \pm 20 nm. The superfluid density ρs(T)=λ2(0)/λ2(T)ρ_s(T)=λ^2(0)/λ^2(T) was fitted with a self-consistent two-gap γ−γ-model. While two different gaps are needed to describe the full-range temperature variation of ρs(T)ρ_s(T), a non-exponential behavior at low temperatures requires additional factors, such as scattering and/or significant gap anisotropy.

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