2012/01/31 by H. Z. Arham, Hamood Z. Arham, C. R. Hunt +26 · 54 citations
Biochemistry, Genetics and Molecular Biology · Materials Science · Physics and Astronomy · #Amyloidosis: Diagnosis, Treatment, Outcomes #Anisotropy #Condensed matter physics #Doping #Electrical engineering #Electrical resistivity and conductivity #Geometry #Iron-based superconductors research #Optics #Physics #Plane (geometry) #Quantum mechanics #Resistive touchscreen #Spectroscopy #cond-mat.supr-con
paper · pdf · doi:10.1103/physrevb.85.214515
published in Physical Review B 85(21) (American Physical Society) · Accepted for publication in Physical Review B
arxiv created 2012/06/04 · openalex publication_date 2012/06/18 · arxiv updated 2016/11/26 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We use point-contact spectroscopy (PCS) to probe AEFe2As2 (AE=Ca,\phantom\rule4.pt0exSr,\phantom\rule4.pt0exBa) and Fe1+yTe. For AE=Sr,Ba we detect orbital fluctuations above TS while for AE=Ca these fluctuations start below TS. Co doping preserves the orbital fluctuations while K doping suppresses it. The fluctuations are only seen at those dopings and temperatures where an in-plane resistive anisotropy is known to exist. We predict an in-plane resistive anisotropy of Fe1+yTe above TS. Our data are examined in light of the recent work by Lee and Phillips (arXiv:1110.5917v2). We also study how joule heating in the PCS junctions impacts the spectra. Spectroscopic information is only obtained from those PCS junctions that are free of heating effects while those PCS junctions that are in the thermal regime display bulk resistivity phenomena.