Abstract

BaFe 2As 2 is the parent compound of the ‘122’ iron arsenide superconductors and crystallizes with the tetragonal ThCr 2Si 2-type structure, space group I4/ mmm. A spin-density-wave transition at 140 K is accompanied by a symmetry reduction to space group Fmmm and simultaneously by antiferromagnetic ordering. Hole-doping induces superconductivity in Ba 1− x K x Fe 2As 2 with a maximum T c of 38 K at x ≈ 0.4. The upper critical fields approach 75 T with rather small anisotropy of H c2. At low potassium concentrations ( x ⩽ 0.2), superconductivity apparently co-exists with the orthorhombically distorted and magnetically ordered phase. At doping levels x ⩾ 0.3, the structural distortion and antiferromagnetic ordering is completely suppressed and the T c is maximized. No magnetically ordered domains could be detected in optimally doped Ba 1− x K x Fe 2As 2 ( x ⩾ 0.3) by 57Fe Mössbauer spectroscopy in contrast μSR results obtained with single crystals. The magnetic hyperfine interactions investigated by 57Fe Mössbauer spectroscopy are discussed and compared to the ZrCuSiAs-type materials.

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