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Superconductivity at 38 K in the Iron Arsenide(Ba1−xKx)Fe2As2

2008/05/31 by M. Rotter, Marianne Rotter, Marcus Tegel +1 · 66 citations
Chemistry · Materials Science · Physics and Astronomy · #Arsenide #Chemistry #Condensed matter physics #Crystal structure #Crystallography #Doping #Gallium arsenide #Ion #Iron-based superconductors research #Materials science #Physics #Quantum mechanics #Rare-earth and actinide compounds #Superconductivity #Ternary operation #Tetragonal crystal system #cond-mat.str-el #cond-mat.supr-con

paper · pdf · doi:10.1103/physrevlett.101.107006

published as Phys. Rev. Lett. 101, 107006 (2008) · 4 pages, 5 figures, submitted to Phys. Rev. Lett

arxiv created 2008/07/17 · openalex publication_date 2008/09/05 · arxiv updated 2009/12/01 · openalex created_date 2020/05/13 · openalex updated_date 2026/08/05

Abstract

The ternary iron arsenide BaFe2As2 becomes superconducting by hole doping, which was achieved by partial substitution of the barium site with potassium. We have discovered bulk superconductivity at Tc=38 K in (Ba_1\ensuremath-xKx)Fe2As2 with x\ensuremath≈0.4. The parent compound BaFe2As2 crystallizes in the tetragonal ThCr2Si2-type structure, which consists of (FeAs)^\ensuremathδ\ensuremath- iron arsenide layers separated by Ba2+ ions. BaFe2As2 is a poor metal and exhibits a spin density wave anomaly at 140 K. By substituting Ba2+ for K+ ions we have introduced holes in the (FeAs)^\ensuremath- layers, which suppress the anomaly and induce superconductivity. The Tc of 38 K in (Ba0.6K0.4)Fe2As2 is the highest in hole doped iron arsenide superconductors so far. Therefore, we were able to expand this class of superconductors by oxygen-free compounds with the ThCr2Si2-type structure.

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