Particle-Hole Asymmetric Ferromagnetism and Spin Textures in the Triangular Hubbard-Hofstadter Model

In a lattice model subject to a perpendicular magnetic field, when the lattice constant is comparable to the magnetic length, one enters the “Hofstadter regime,” where continuum Landau levels become fractal magnetic Bloch bands. Strong mixing between bands alters the nature of the resulting quantum phases compared to the continuum limit; lattice potential, magnetic field, and Coulomb interaction must be treated on equal footing. Using determinant quantum Monte Carlo and density matrix renormalization group techniques, we study this regime numerically in the context of the Hubbard-Hofstadter model on a triangular lattice. In the field-filling phase diagram, we find a broad wedge-shaped region of ferromagnetic ground states for filling factor <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>ν</a:mi><a:mo>≤</a:mo><a:mn>1</a:mn></a:math>, bounded below by filling factor <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>ν</c:mi><c:mo>=</c:mo><c:mn>1</c:mn></c:math> and bounded above by half filling the lowest Hofstadter subband. We observe signatures of SU(2) quantum Hall ferromagnetism at filling factors <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>ν</e:mi><e:mo>=</e:mo><e:mn>1</e:mn></e:math> and <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mi>ν</g:mi><g:mo>=</g:mo><g:mn>3</g:mn></g:math>. The phases near <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:mi>ν</i:mi><i:mo>=</i:mo><i:mn>1</i:mn></i:math> are particle-hole asymmetric, and we observe a rapid decrease in ground-state spin polarization consistent with the formation of skyrmions only on the electron doped side. At large fields, above the ferromagnetic wedge, we observe a low-spin metallic region with spin correlations peaked at small momenta. We argue that the phenomenology of this region likely results from exchange interaction mixing fractal Hofstadter subbands. The phase diagram derived beyond the continuum limit points to a rich landscape to explore interaction effects in magnetic Bloch bands. Published by the American Physical Society 2024

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Journal
Physical Review X
Published
2024-10-25
DOI
https://doi.org/10.1103/physrevx.14.041025
Citations
7
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
Field-Weighted Citation Impact
2.18

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article

Particle-Hole Asymmetric Ferromagnetism and Spin Textures in the Triangular Hubbard-Hofstadter Model

Luhang Yang, Ziyan Zhu, Edwin W. Huang, Peizhi Mai et al.
7 citations
Physical Review X
Physics of Superconductivity and Magnetism
2.18
article

Particle-Hole Asymmetric Ferromagnetism and Spin Textures in the Triangular Hubbard-Hofstadter Model

Luhang Yang, Ziyan Zhu, Edwin W. Huang, Peizhi Mai, Philip Phillips, Thomas Devereaux, Benjamin E. Feldman, Wen O. Wang, Brian Moritz, Jixun K. Ding, Peng Cheng
article en
7 citations

Abstract

In a lattice model subject to a perpendicular magnetic field, when the lattice constant is comparable to the magnetic length, one enters the “Hofstadter regime,” where continuum Landau levels become fractal magnetic Bloch bands. Strong mixing between bands alters the nature of the resulting quantum phases compared to the continuum limit; lattice potential, magnetic field, and Coulomb interaction must be treated on equal footing. Using determinant quantum Monte Carlo and density matrix renormalization group techniques, we study this regime numerically in the context of the Hubbard-Hofstadter model on a triangular lattice. In the field-filling phase diagram, we find a broad wedge-shaped region of ferromagnetic ground states for filling factor <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>ν</a:mi><a:mo>≤</a:mo><a:mn>1</a:mn></a:math>, bounded below by filling factor <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>ν</c:mi><c:mo>=</c:mo><c:mn>1</c:mn></c:math> and bounded above by half filling the lowest Hofstadter subband. We observe signatures of SU(2) quantum Hall ferromagnetism at filling factors <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>ν</e:mi><e:mo>=</e:mo><e:mn>1</e:mn></e:math> and <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:mi>ν</g:mi><g:mo>=</g:mo><g:mn>3</g:mn></g:math>. The phases near <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:mi>ν</i:mi><i:mo>=</i:mo><i:mn>1</i:mn></i:math> are particle-hole asymmetric, and we observe a rapid decrease in ground-state spin polarization consistent with the formation of skyrmions only on the electron doped side. At large fields, above the ferromagnetic wedge, we observe a low-spin metallic region with spin correlations peaked at small momenta. We argue that the phenomenology of this region likely results from exchange interaction mixing fractal Hofstadter subbands. The phase diagram derived beyond the continuum limit points to a rich landscape to explore interaction effects in magnetic Bloch bands. Published by the American Physical Society 2024

Physical Review XVol. 14(4)
University of Notre Dame (US), Northeastern University (US), University of Illinois Urbana-Champaign (US), SLAC National Accelerator Laboratory (US), Universidad del Noreste (MX), Stanford University (US)
U.S. Department of Energy, Gordon and Betty Moore Foundation, Stanford University, National Energy Research Scientific Computing Center, Office of Science, Basic Energy Sciences, Energy Frontier Research Centers, Division of Materials Sciences and Engineering
Sustainable cities and communities
Openalex Percentile: Top 12%
Physics of Superconductivity and Magnetism
2.18
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