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Temperature dependence of the superconducting energy gaps in Ca9.35La0.65(Pt3As8)(Fe2As2)5 single crystal

机译:Ca9.35La0.65(Pt3As8)(Fe2As2)5单晶中超导能隙的温度依赖性

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摘要

We measured the optical reflectivity R(ω) for an underdoped (Ca0.935La0.065)10(Pt3As8)(Fe2As2)5 single crystal and obtained the optical conductivity σ1(ω) using the K-K transformation. The normal state σ1(ω) at 30 K is well fitted by a Drude-Lorentz model with two Drude components (ωp1 = 1446 cm−1 and ωp2 = 6322 cm−1) and seven Lorentz components. Relative reflectometry was used to accurately determine the temperature dependence of the superconducting gap at various temperatures below Tc. The results clearly show the opening of a superconducting gap with a weaker second gap structure; the magnitudes for the gaps are estimated from the generalized Mattis-Bardeen model to be Δ1 = 30 and Δ2 = 50 cm−1, respectively, at T = 8 K, which both decrease with increasing temperature. The temperature dependence of the gaps was not consistent with one-band BCS theory but was well described by a two-band (hence, two gap) BCS model with interband interactions. The temperature dependence of the superfluid density is flat at low temperatures, indicating an s-wave full-gap superconducting state.
机译:我们测量了掺杂不足的(Ca0.935La0.065)10(Pt3As8)(Fe2As2)5单晶的光反射率R(ω),并使用K-K变换获得了光导率σ1(ω)。具有两个Drude分量(ωp1= 1446 cm -1 和ωp2= 6322 cm -1 )和七个Lorentz组件。相对反射法用于精确确定低于Tc的各种温度下超导间隙的温度依赖性。结果清楚地表明,具有较弱第二间隙结构的超导间隙的打开;根据广义Mattis-Bardeen模型估计,在T = 8 K时,间隙的大小分别为Δ1= 30和Δ2= 50 cm -1 ,它们均随温度升高而降低。间隙的温度依赖性与单频带BCS理论不一致,但可以通过具有频带间相互作用的两频带(因此为两个间隙)BCS模型很好地描述。在低温下,超流体密度的温度依赖性是平坦的,表明s波为全间隙超导状态。

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