Atomic-scale distortions and temperature-dependent large pseudogap in thin films of the parent iron-chalcogenide superconductor Fe1+yTe. (9th November 2017)

• Record Type: Journal Article
• Authors: Gerbi, Andrea; Buzio, Renato; Kawale, Shrikant; Bellingeri, Emilio; Martinelli, Alberto; Bernini, Cristina; Tresca, Cesare; Capone, Massimo; Profeta, Gianni; Ferdeghini, Carlo
• Is Part Of: Journal of physics. Volume 29:Number 48(2017)
• Publication Date: 2017-11-09
• Subjects: scanning tunneling of surfaces, interfaces, and thin films 68.37.Yz -- scanning tunneling microscopes 07.79.Fc -- superconducting materials chalcogenides 74.70.Xa -- thin films 73.50. −h, 73.61. −r -- strongly correlated electron systems 71.27. + a -- laser deposition 81.15.Fg; Condensed matter -- Periodicals; Matière condensée -- Périodiques; Vaste stoffen; Vloeistoffen; Natuurkunde; Electronic journals; Computer network resources; 530.4105
• DOI: 10.1088/1361-648X/aa9103
• Languages: English
• ISSNs: 0953-8984

Abstract

Abstract: We investigate with scanning tunneling microscopy/spectroscopy (STM/STS) and density functional theory (DFT) calculations the surface structures and the electronic properties of Fe1+ y Te thin films grown by pulsed laser deposition. Contrary to the regular arrangement of antiferromagnetic nanostripes previously reported on cleaved single-crystal samples, the surface of Fe1+ y Te thin films displays a peculiar distribution of spatially inhomogeneous nanostripes. Both STM and DFT calculations show the bias-dependent nature of such features and support the interpretation of spin-polarized tunneling between the FeTe surface and an unintentionally magnetized tip. In addition, the spatial inhomogeneity is interpreted as a purely electronic effect related to changes in hybridization and Fe–Fe bond length driven by local variations in the concentration of excess interstitial Fe cations. Unexpectedly, the surface density of states measured by STS strongly evolves with temperature in close proximity to the antiferromagnetic–paramagnetic first-order transition, and reveals a large pseudogap of 180–250 meV at about 50–65 K. We believe that in this temperature range a phase transition takes place, and the system orders and locks into particular combinations of orbitals and spins because of the interplay between excess interstitial magnetic Fe and strongly correlated d -electrons.