Superconducting properties and pseudogap from preformed Cooper pairs in the triclinic (CaFe1−x_{1-x}Ptx_xAs)10_{10}Pt3_3As8_8

preprint2014arXivOpen access

Abstract

Using a combination of muon-spin relaxation (μμSR), inelastic neutron scattering (INS) and nuclear magnetic resonance (NMR), we investigated the novel iron-based superconductor with a triclinic crystal structure (CaFe1−x_{1-x}Ptx_xAs)10_{10}Pt3_3As8_8 (Tc_{\rm c} = 13 K), containing platinum-arsenide intermediary layers. The temperature dependence of the superfluid density obtained from the μμSR relaxation-rate measurements indicates the presence of two superconducting gaps, Δ1≫Δ2Δ_\text{1}\ggΔ_\text{2}. According to our INS measurements, commensurate spin fluctuations are centered at the (ππ, 0) wave vector, like in most other iron arsenides. Their intensity remains unchanged across Tc_\text{c}, indicating the absence of a spin resonance typical for many Fe-based superconductors. Instead, we observed a peak in the spin-excitation spectrum around ℏω0= \hslashω_0=\,7 meV at the same wave vector, which persists above Tc_{\rm c} and is characterized by the ratio ℏω0/kBTc≈ \hslashω_0/k_\text{B}T_\text{c}\approx\,6.2, which is significantly higher than typical values for the magnetic resonant modes in iron pnictides (~4.3). The temperature dependence of magnetic intensity at 7 meV revealed an anomaly around T* = 45 K related to the disappearance of this new mode. A suppression of the spin-lattice relaxation rate, 1/T1T1/T_1T, observed by NMR immediately below T* without any notable subsequent anomaly at Tc_{\rm c}, indicates that T* could mark the onset of a pseudogap in (CaFe1−x_{1-x}Ptx_xAs)10_{10}Pt3_3As8_8, which is likely associated with the emergence of preformed Cooper pairs.

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