Canted magnetism and $\mathbb{Z}_2$ fractionalization in metallic states of the Lieb lattice Hubbard model near quarter filling

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Main Authors: Nikolaenko, Alexander, Bonetti, Pietro M., Kale, Anant, Lebrat, Martin, Greiner, Markus, Sachdev, Subir
Format: Preprint
Published: 2025
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author Nikolaenko, Alexander
Bonetti, Pietro M.
Kale, Anant
Lebrat, Martin
Greiner, Markus
Sachdev, Subir
author_facet Nikolaenko, Alexander
Bonetti, Pietro M.
Kale, Anant
Lebrat, Martin
Greiner, Markus
Sachdev, Subir
contents A recent experiment has examined ultracold, fermionic, spin-1/2 $^6$Li atoms in the Lieb lattice at different Hubbard repulsion $U$ and filling fractions $ν$ (Lebrat et al. arXiv:2404.17555). At $ν=1/2$ and small $U$, they observe an enhanced compressibility on the $p_{x,y}$ sites, pointing to a flat band near the Fermi energy. At $ν=1/2$ and large $U$ they observe an insulating ferrimagnet. Both small and large $U$ observations at $ν=1/2$ are consistent with theoretical expectations. Surprisingly, near $ν=1/4$ and large $U$, they again observe a large $p_{x,y}$ compressibility, pointing to a flat $p_{x,y}$ band of fermions across the Fermi energy. Our Hartree-Fock computations near $ν=1/4$ find states with canted magnetism (and related spiral states) at large $U$, which possess nearly flat $p_{x,y}$ bands near the Fermi level. We employ parton theories to describe quantum fluctuations of the magnetic order found in Hartree-Fock. We find a metallic state with $\mathbb{Z}_2$ fractionalization possessing gapless, fermionic, spinless `chargons' carrying $\mathbb{Z}_2$ gauge charges which have a nearly flat $p_{x,y}$ band near their Fermi level: this fractionalized metal is also consistent with observations. Our DMRG study does not indicate the presence of magnetic order, and so supports a fractionalized ground state. Given the conventional ferrimagnetic insulator at $ν=1/2$, the $\mathbb{Z}_2$ fractionalized metal at $ν=1/4$ represents a remarkable realization of doping-induced fractionalization.
format Preprint
id arxiv_https___arxiv_org_abs_2502_12235
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Canted magnetism and $\mathbb{Z}_2$ fractionalization in metallic states of the Lieb lattice Hubbard model near quarter filling
Nikolaenko, Alexander
Bonetti, Pietro M.
Kale, Anant
Lebrat, Martin
Greiner, Markus
Sachdev, Subir
Strongly Correlated Electrons
Quantum Gases
A recent experiment has examined ultracold, fermionic, spin-1/2 $^6$Li atoms in the Lieb lattice at different Hubbard repulsion $U$ and filling fractions $ν$ (Lebrat et al. arXiv:2404.17555). At $ν=1/2$ and small $U$, they observe an enhanced compressibility on the $p_{x,y}$ sites, pointing to a flat band near the Fermi energy. At $ν=1/2$ and large $U$ they observe an insulating ferrimagnet. Both small and large $U$ observations at $ν=1/2$ are consistent with theoretical expectations. Surprisingly, near $ν=1/4$ and large $U$, they again observe a large $p_{x,y}$ compressibility, pointing to a flat $p_{x,y}$ band of fermions across the Fermi energy. Our Hartree-Fock computations near $ν=1/4$ find states with canted magnetism (and related spiral states) at large $U$, which possess nearly flat $p_{x,y}$ bands near the Fermi level. We employ parton theories to describe quantum fluctuations of the magnetic order found in Hartree-Fock. We find a metallic state with $\mathbb{Z}_2$ fractionalization possessing gapless, fermionic, spinless `chargons' carrying $\mathbb{Z}_2$ gauge charges which have a nearly flat $p_{x,y}$ band near their Fermi level: this fractionalized metal is also consistent with observations. Our DMRG study does not indicate the presence of magnetic order, and so supports a fractionalized ground state. Given the conventional ferrimagnetic insulator at $ν=1/2$, the $\mathbb{Z}_2$ fractionalized metal at $ν=1/4$ represents a remarkable realization of doping-induced fractionalization.
title Canted magnetism and $\mathbb{Z}_2$ fractionalization in metallic states of the Lieb lattice Hubbard model near quarter filling
topic Strongly Correlated Electrons
Quantum Gases
url https://arxiv.org/abs/2502.12235