Weyl semimetallic, Néel, spiral, and vortex states in the Rashba-Hubbard model

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Main Authors: Sousa-Júnior, Sebastião dos Anjos, Mondaini, Rubem
Format: Preprint
Published: 2025
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author Sousa-Júnior, Sebastião dos Anjos
Mondaini, Rubem
author_facet Sousa-Júnior, Sebastião dos Anjos
Mondaini, Rubem
contents We investigate the evolution of magnetic phases in the Hubbard model under strong Rashba spin-orbit coupling on a square lattice. By using Lanczos exact diagonalization and determinant quantum Monte Carlo (DQMC) simulations, we explore the emergence of various magnetic alignments as the ratio between the regular hopping amplitude, $t$, and the Rashba hopping term, $t_R$, is varied over a broad range of Hubbard interaction strengths, $U$. In the limit $t_R \rightarrow 0$, the system exhibits Néel antiferromagnetic order, while when $t \sim t_R$, a spiral magnetic phase emerges due to the induced anisotropic Dzyaloshinskii-Moriya interaction. For $t_R > t$, we identify the onset of a spin vortex phase. At the extreme limit $t = 0$($t_R \neq 0 $), we perform finite-size scaling analysis in the Weyl semimetal regime to pinpoint the quantum critical point associated with the spin vortex phase, employing sign-free quantum Monte Carlo simulations - the extracted critical exponents are consistent with a Gross-Neveu-type quantum phase transition.
format Preprint
id arxiv_https___arxiv_org_abs_2501_01590
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Weyl semimetallic, Néel, spiral, and vortex states in the Rashba-Hubbard model
Sousa-Júnior, Sebastião dos Anjos
Mondaini, Rubem
Strongly Correlated Electrons
We investigate the evolution of magnetic phases in the Hubbard model under strong Rashba spin-orbit coupling on a square lattice. By using Lanczos exact diagonalization and determinant quantum Monte Carlo (DQMC) simulations, we explore the emergence of various magnetic alignments as the ratio between the regular hopping amplitude, $t$, and the Rashba hopping term, $t_R$, is varied over a broad range of Hubbard interaction strengths, $U$. In the limit $t_R \rightarrow 0$, the system exhibits Néel antiferromagnetic order, while when $t \sim t_R$, a spiral magnetic phase emerges due to the induced anisotropic Dzyaloshinskii-Moriya interaction. For $t_R > t$, we identify the onset of a spin vortex phase. At the extreme limit $t = 0$($t_R \neq 0 $), we perform finite-size scaling analysis in the Weyl semimetal regime to pinpoint the quantum critical point associated with the spin vortex phase, employing sign-free quantum Monte Carlo simulations - the extracted critical exponents are consistent with a Gross-Neveu-type quantum phase transition.
title Weyl semimetallic, Néel, spiral, and vortex states in the Rashba-Hubbard model
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2501.01590