Observation of universal strong orbital-dependent correlation effects in iron chalcogenides

Ming Yi(SLAC National Accelerator Laboratory), Z-K Liu(SLAC National Accelerator Laboratory), Yi Zhang(Lawrence Berkeley National Laboratory), Rong Yu(Rice University), Jian‐Xin Zhu(Los Alamos National Laboratory), J. J. Lee(SLAC National Accelerator Laboratory), R. G. Moore(SLAC National Accelerator Laboratory), F. Schmitt(SLAC National Accelerator Laboratory), W. Li(SLAC National Accelerator Laboratory), Scott Riggs(SLAC National Accelerator Laboratory), Jin Chu(SLAC National Accelerator Laboratory), Bing Lv(University of Houston), Jin Hu(Tulane University), M. Hashimoto(SLAC National Accelerator Laboratory), Sung‐Kwan Mo(Lawrence Berkeley National Laboratory), Z. Hussain(Lawrence Berkeley National Laboratory), Zhiqiang Mao(Tulane University), C. W. Chu(University of Houston), I. R. Fisher(SLAC National Accelerator Laboratory), Qimiao Si(Rice University), Zhi‐Xun Shen(SLAC National Accelerator Laboratory), Dong-Hui Lu(SLAC National Accelerator Laboratory)
Nature Communications
July 23, 2015
Cited by 201Open Access
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Abstract

Establishing the appropriate theoretical framework for unconventional superconductivity in the iron-based materials requires correct understanding of both the electron correlation strength and the role of Fermi surfaces. This fundamental issue becomes especially relevant with the discovery of the iron chalcogenide superconductors. Here, we use angle-resolved photoemission spectroscopy to measure three representative iron chalcogenides, FeTe0.56Se0.44, monolayer FeSe grown on SrTiO3 and K0.76Fe1.72Se2. We show that these superconductors are all strongly correlated, with an orbital-selective strong renormalization in the dxy bands despite having drastically different Fermi surface topologies. Furthermore, raising temperature brings all three compounds from a metallic state to a phase where the dxy orbital loses all spectral weight while other orbitals remain itinerant. These observations establish that iron chalcogenides display universal orbital-selective strong correlations that are insensitive to the Fermi surface topology, and are close to an orbital-selective Mott phase, hence placing strong constraints for theoretical understanding of iron-based superconductors.


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