FeSe superconductivity is controlled by Hund's coupling strength and the proximity of the Fe dxy orbital to the Fermi level, with the monolayer on SrTiO3 naturally realizing a near-optimal combination.
Simultaneous emergence of superconductivity, inter-pocket scattering and nematic fluctuation in potassium-coated FeSe superconductor
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abstract
Superconductivity originates from pairing of electrons. Pairing channel on Fermi surface and pairing glue are thus two pivotal issues for understanding a superconductor. Recently, high-temperature superconductivity over 40 K was found in electron-doped FeSe superconductors including K$_x$Fe$_{2-y}$Se$_2$, Li$_{0.8}$Fe$_{0.2}$OHFeSe, and 1 monolayer FeSe thin film. However, their pairing mechanism remains controversial. Here, we studied the systematic evolution of electronic structure in potassium-coated FeSe single crystal. The doping level is controlled precisely by in situ evaporating potassium onto the sample surface. We found that the superconductivity emerges when the inter-pocket scattering between two electron pockets is turned on by a Lifshitz transition of Fermi surface. The nematic order suppresses remarkably at the same doping and strong nematic fluctuation remains in a wide doping range of the phase diagram. Our results suggest an underlying correlation among superconductivity, inter-pocket scattering, and nematic fluctuation in electron-doped FeSe superconductors.
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cond-mat.str-el 1years
2019 1verdicts
CONDITIONAL 1representative citing papers
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Interplay between band structure and Hund's correlation to increase T$_{c}$ in FeSe
FeSe superconductivity is controlled by Hund's coupling strength and the proximity of the Fe dxy orbital to the Fermi level, with the monolayer on SrTiO3 naturally realizing a near-optimal combination.