Ferromagnetically ordered states in the Hubbard model on the $H_{00}$ hexagonal golden-mean tiling

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Hauptverfasser: Matsubara, Toranosuke, Koga, Akihisa, Coates, Sam
Format: Preprint
Veröffentlicht: 2023
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author Matsubara, Toranosuke
Koga, Akihisa
Coates, Sam
author_facet Matsubara, Toranosuke
Koga, Akihisa
Coates, Sam
contents We study magnetic properties of the half-filled Hubbard model on the two-dimensional $H_{00}$ hexagonal golden-mean quasiperiodic tiling. The tiling is composed of large and small hexagons, and parallelograms, and its vertex model is bipartite with a sublattice imbalance. The tight-binding model on the tiling has macroscopically degenerate states at $E = 0$. We find the existence of two extended states in one of the sublattices, in addition to confined states in the other. This property is distinct from that of the well-known two-dimensional quasiperiodic tilings such as the Penrose and Ammann-Beenker tilings. Applying the Lieb theorem to the Hubbard model on the tiling, we obtain the exact fraction of the confined states as $1/2τ^2$, where $τ$ is the golden mean. This leads to a ferromagnetically ordered state in the weak coupling limit. Increasing the Coulomb interaction, the staggered magnetic moments are induced and gradually increase. Crossover behaviour in the magnetically ordered states is also addressed in terms of perpendicular space analysis.
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id arxiv_https___arxiv_org_abs_2306_15200
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Ferromagnetically ordered states in the Hubbard model on the $H_{00}$ hexagonal golden-mean tiling
Matsubara, Toranosuke
Koga, Akihisa
Coates, Sam
Strongly Correlated Electrons
We study magnetic properties of the half-filled Hubbard model on the two-dimensional $H_{00}$ hexagonal golden-mean quasiperiodic tiling. The tiling is composed of large and small hexagons, and parallelograms, and its vertex model is bipartite with a sublattice imbalance. The tight-binding model on the tiling has macroscopically degenerate states at $E = 0$. We find the existence of two extended states in one of the sublattices, in addition to confined states in the other. This property is distinct from that of the well-known two-dimensional quasiperiodic tilings such as the Penrose and Ammann-Beenker tilings. Applying the Lieb theorem to the Hubbard model on the tiling, we obtain the exact fraction of the confined states as $1/2τ^2$, where $τ$ is the golden mean. This leads to a ferromagnetically ordered state in the weak coupling limit. Increasing the Coulomb interaction, the staggered magnetic moments are induced and gradually increase. Crossover behaviour in the magnetically ordered states is also addressed in terms of perpendicular space analysis.
title Ferromagnetically ordered states in the Hubbard model on the $H_{00}$ hexagonal golden-mean tiling
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2306.15200