Point-contact spectroscopic studies on normal and superconducting AFe 2As2-type iron pnictide single crystals

  • Xin Lu
  • , W. K. Park
  • , H. Q. Yuan
  • , G. F. Chen
  • , G. L. Luo
  • , N. L. Wang
  • , A. S. Sefat
  • , M. A. McGuire
  • , R. Jin
  • , B. C. Sales
  • , D. Mandrus
  • , J. Gillett
  • , Suchitra E. Sebastian
  • , L. H. Greene

Research output: Contribution to journalArticlepeer-review

30 Scopus citations

Abstract

Point-contact Andreev reflection spectroscopy is applied to investigate the gap structure in iron pnictide single-crystal superconductors of the AFe 2As2 (A = Ba, Sr) family ('Fe-122'). The observed point-contact junction conductance curves, G(V), can be divided into two categories: one where Andreev reflection is present for both (Ba 0.6K0.4)Fe2As2 and Ba(Fe 0.9Co0.1)2As2, and the other with a V2/3 background conductance universally observed, extending even up to 100meV for Sr0.6Na0.4Fe2As2 and Sr(Fe0.9Co0.1)2As2. The latter is also observed in point-contact junctions on the nonsuperconducting parent compound BaFe2As2 and superconducting (Ba 0.6K0.4)Fe2As2 crystals. Mesoscopic phase-separated coexistence of magnetic and superconducting orders is considered to explain distinct behaviors in the superconducting samples. For Ba 0.6K0.4Fe2As2, double peaks due to Andreev reflection with a strongly sloping background are frequently observed for point contacts on freshly cleaved c-axis surfaces. If normalized using a background baseline and analyzed using the Blonder-Tinkham-Klapwijk model, the data show a gap size of ∼ 3.0-4.0meV with 2Δ0/k BTc ∼ 2.0-2.6, consistent with the smaller gap size reported for the LnFeAsO family ('Fe-1111'). For the Ba(Fe0.9Co 0.1)2As2, the G(V) curves typically display a zero-bias conductance peak.

Original languageEnglish
Article number054009
JournalSuperconductor Science and Technology
Volume23
Issue number5
DOIs
StatePublished - 2010

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