Effect of Electron-Electron Interactions on Metallic State in Quasicrystals
arXiv:2008.07100 · doi:10.2320/matertrans.MT-MB2020001
Abstract
We theoretically study the effect of electron-electron interactions on the metallic state of quasicrystals. To address the problem, we introduce the extended Hubbard model on the Ammann-Beenker tiling as a simple theoretical model. The model is numerically solved within an inhomogeneous mean-field theory. Because of the lack of periodicity, the metallic state is nonuniform in the electron density even in the noninteracting limit. We clarify how this charge distribution pattern changes with electron-electron interactions. We find that the intersite interactions change the distribution substantially and in an electron-hole asymmetric way. We clarify the origin of these changes through the analyses in the real and perpendicular spaces. Our results offer a fundamental basis to understand the electronic states in quasicrystalline metals.
9 pages, 5 figures
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- The Kernel Polynomial Method
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- Supercurrent Distribution in Real-Space and Anomalous Paramagnetic Response in a Superconducting Quasicrystal
- Doped Mott insulator on Penrose tiling
- Hyperuniformity in two-dimensional periodic and quasiperiodic point patterns
- Self-consistent study of topological superconductivity in two-dimensional quasicrystals
- Ferromagnetically ordered states in the Hubbard model on the hexagonal golden-mean tiling
- Superconductivity and charge-density-wave in the Holstein model on the Penrose Lattice
- Hyperuniform properties of the square-triangle tilings
- Non-Collinear and Non-Coplanar Magnetic Orders in 1/1 Periodic Approximant to the Icosahedral Quasicrystal
- Magnetism and topological property in icosahedral quasicrystal
- Optical response of the tightbinding model on the Fibonacci chain
- Mott transition and correlation effects on strictly localized states in an octagonal quasicrystal