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Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
Published on: June 9, 2023
Band Structure of Organic-Ion-Intercalated (EMIM)FeSe Superconductor
Lyudmila V Begunovich1, Maxim M Korshunov1,2
1Siberian Federal University, Svobodny Prospect 79, 660041 Krasnoyarsk, Russia.
Density functional theory reveals that iron (Fe) d-orbitals primarily form bands in the superconductor (EMIM)xFeSe. Organic cations shift the chemical potential, creating electron pockets in the Fermi surface.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Solid State Chemistry
Background:
- Superconductivity in iron-based materials is a significant area of research.
- Understanding the electronic structure is crucial for designing new superconductors.
- The role of organic components in inorganic superconductors is not fully understood.
Purpose of the Study:
- To investigate the electronic band structure and Fermi surface of the novel superconductor (EMIM)xFeSe.
- To elucidate the contribution of different atomic orbitals to the electronic states near the Fermi level.
- To determine the influence of the organic cation (EMIM) on the superconducting properties.
Main Methods:
- Utilizing density functional theory (DFT) calculations.
- Employing the generalized gradient approximation (GGA) for exchange-correlation functional.
- Analyzing the band structure and Fermi surface topology.
Main Results:
- The bands near the Fermi level are predominantly derived from Fe-d orbitals.
- No direct contribution from EMIM orbitals to the near-Fermi level states was found.
- The presence of EMIM cations causes a chemical potential shift.
- Small electron pockets emerge on the quasi-two-dimensional Fermi surface.
Conclusions:
- The electronic properties of (EMIM)xFeSe are mainly governed by Fe-d states.
- The organic component plays a crucial indirect role by modulating the electronic structure.
- The formation of electron pockets is a key feature of this superconductor's Fermi surface.
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