Superconductivity across Lifshitz transition and anomalous insulating state in surface K-dosed (Li0.8Fe0.2OH)FeSe
arXiv:1708.05635 · doi:10.1126/sciadv.1603238
Abstract
In the iron-based superconductors, understanding the relation between superconductivity and electronic structure upon doping is crucial for exploring the pairing mechanism. Recently it was found that in iron selenide (FeSe), enhanced superconductivity (Tc over 40K) can be achieved via electron doping, with the Fermi surface only comprising M-centered electron pockets. Here by utilizing surface potassium dosing, scanning tunneling microscopy/spectroscopy (STM/STS) and angle-resolved photoemission spectroscopy (ARPES), we studied the electronic structure and superconductivity of (Li0.8Fe0.2OH)FeSe in the deep electron-doped regime. We find that a Γ-centered electron band, which originally lies above the Fermi level (EF), can be continuously tuned to cross EF and contribute a new electron pocket at Γ. When this Lifshitz transition occurs, the superconductivity in the M-centered electron pocket is slightly suppressed; while a possible superconducting gap with small size (up to ~5 meV) and a dome-like doping dependence is observed on the new Γ electron pocket. Upon further K dosing, the system eventually evolves into an insulating state. Our findings provide new clues to understand superconductivity versus Fermi surface topology and the correlation effect in FeSe-based superconductors.
21 pages, 13 figures
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- Charge order driven by multiple-Q spin fluctuations in heavily electron-doped iron selenide superconductors
- Ultrafast dynamics in the Lifshitz-type 5 pyrochlore antiferromagnet CdOsO
- Enhanced Surface Superconductivity in Ba(FeCo)As
- Spin correlations in the parent phase of LiFeODFeSe
- Incommensurate spin fluctuations and competing pairing symmetries in LaNiO
- Higher-Order Topology in Monolayer FeSe