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20 April 2024
 
  » arxiv » 1506.2875

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Fluctuation conductivity and possible pseudogap state in FeAs-based superconductor EuFeAsO(0.85)F(0.15)
A. L. Solovjov ; L. V. Omelchenko ; A. V.Terekhov ; E.P. Khlybov ; K. Rogacki ;
Date 9 Jun 2015
AbstractThe study of excess conductivity $sigma’(T)$ in the textured polycrystalline FeAs-based superconductor $EuFeAsO_{0.85}F_{0.15}$ ($T_c = 11, K$) prepared by the solid state synthesis is reported. The $sigma’(T)$ analysis has been performed within the Local Pair (LP) model based on the assumption of the LP formation in cuprate high-$T_c$ superconductors (cuprates) below the pseudogap (PG) temperature $T^*gg T_c$. Similarly to the cuprates, near $T_c$ $sigma’(T)$ is adequately described by the 3D term of the Aslamasov-Larkin (AL) theory but the range of the 3D-AL fluctuations, $Delta T_{3D}$, is relatively short. Above the crossover temperature $T_0 approx 11.7,K$ $sigma’(T)$ is described by the 2D Maki-Thompson (MT) fluctuation term of the Hikami-Larkin (HL) theory. But enhanced 2D-MT fluctuation contribution, being typical for the magnetic superconductors, is observed. Within the LP model approach the PG parameter, $Delta^*(T)$, was determined for the first time. $Delta^*(T)$ shows the narrow maximum at $T_s approx 160,K$ followed by the linear drop down to $T_{SDW}=T_{NFe}approx 133,K$. Both small $Delta T_{3D}$ and enhanced $sigma’(T)$, including linear $Delta^*(T)$ drop, are considered to be the evidence of the enhanced magnetic interaction in $EuFeAsO_{0.85}F_{0.15}$. Importantly, the slop of the linear $Delta^*(T)$ and its length are found to be the same as observed for $SmFeAsO_{0.85}$. The results suggest both the similarity of magnetic interaction processes in different Fe-pnictides and applicability of the LP model approach to the $sigma’(T)$ analysis even in magnetic superconductors.
Source arXiv, 1506.2875
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