Abstract

We report on the temperature dependence of the in plane magnetic penetration depth (λabλ_{ab}) and first penetration field (Hf∝1/λab2(T)H_f\propto 1/λ_{ab}^2(T) for H∥cH\|c) in 2H-NbS2_2 single crystals. An exponential temperature dependence is clearly observed in λabλ_{ab}(T) at low temperature, signing the presence of a fully open superconducting gap. This compound is the only superconducting 2H-dichalcogenide which does not develop a charge density wave (CDW). However as previously observed in 2H-NbSe2_2, this gap (Δ1=1.1 kBTcΔ_{1}=1.1\, k_{B}T_{c}) is significantly smaller than the standard BCS weak coupling value. At higher temperature, a larger gap (Δ2=1.8 kBTcΔ_{2}=1.8\, k_{B}T_{c}) has to be introduced to describe the data which are compatible with a two gap model. The superconducting gaps are hence very similar in NbS2_2 and NbSe2_2 and we show here that both of them open in the strongly coupled Nb tubular sheets independently of the presence of a CDW or not.

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