Topological phonons in anomalous Hall crystals | Matter42 Literature
Paper details
Research paper
Theoretical
Topological phonons in anomalous Hall crystals
Mark R. Hirsbrunner, Félix Desrochers, Joe Huxford, Yong Baek Kim
arXiv preprint·2026·arXiv:2601.06246
Samples
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Continuum infinite Chern band model analyzed at rs = 10 with self-consistent Hartree-Fock followed by TDHF collective-mode calculations for several values of Berry flux through the first Brillouin zone.
No measurements recorded
Simulatedinfinite Chern band modelStudied Material
Continuum λ-jellium model analyzed with self-consistent Hartree-Fock and TDHF collective-mode calculations, including the effect of varying the Berry curvature scale parameter λ.
No measurements recorded
Simulatedλ-jellium modelStudied Material
Weak periodic potential added as a perturbation to test the robustness of collective-mode topology in the anomalous Hall crystal phase.
No measurements recorded
Simulatedweak periodic potentialStudied Material
Materials
infinite Chern band model
Studied Material
Also known as
infinite Chern band
Variables
model_type= ideal quantum geometry continuum model
Berry_curvature= constant
studied material
λ-jellium model
Studied Material
Paper details
Research paper
Theoretical
Topological phonons in anomalous Hall crystals
Mark R. Hirsbrunner, Félix Desrochers, Joe Huxford, Yong Baek Kim
arXiv preprint·2026·arXiv:2601.06246
Samples
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Continuum infinite Chern band model analyzed at rs = 10 with self-consistent Hartree-Fock followed by TDHF collective-mode calculations for several values of Berry flux through the first Brillouin zone.
No measurements recorded
Simulatedinfinite Chern band modelStudied Material
Continuum λ-jellium model analyzed with self-consistent Hartree-Fock and TDHF collective-mode calculations, including the effect of varying the Berry curvature scale parameter λ.
No measurements recorded
Simulatedλ-jellium modelStudied Material
Weak periodic potential added as a perturbation to test the robustness of collective-mode topology in the anomalous Hall crystal phase.
No measurements recorded
Simulatedweak periodic potentialStudied Material
Materials
infinite Chern band model
Studied Material
Also known as
infinite Chern band
Variables
model_type= ideal quantum geometry continuum model
Berry_curvature= constant
studied material
λ-jellium model
Studied Material
Paper details
Research paper
Theoretical
Topological phonons in anomalous Hall crystals
Mark R. Hirsbrunner, Félix Desrochers, Joe Huxford, Yong Baek Kim
arXiv preprint·2026·arXiv:2601.06246
Samples
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Continuum infinite Chern band model analyzed at rs = 10 with self-consistent Hartree-Fock followed by TDHF collective-mode calculations for several values of Berry flux through the first Brillouin zone.
No measurements recorded
Simulatedinfinite Chern band modelStudied Material
Continuum λ-jellium model analyzed with self-consistent Hartree-Fock and TDHF collective-mode calculations, including the effect of varying the Berry curvature scale parameter λ.
No measurements recorded
Simulatedλ-jellium modelStudied Material
Weak periodic potential added as a perturbation to test the robustness of collective-mode topology in the anomalous Hall crystal phase.
No measurements recorded
Simulatedweak periodic potentialStudied Material
Materials
infinite Chern band model
Studied Material
Also known as
infinite Chern band
Variables
model_type= ideal quantum geometry continuum model
Berry_curvature= constant
studied material
λ-jellium model
Studied Material
Paper details
Research paper
Theoretical
Topological phonons in anomalous Hall crystals
Mark R. Hirsbrunner, Félix Desrochers, Joe Huxford, Yong Baek Kim
arXiv preprint·2026·arXiv:2601.06246
Samples
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Continuum infinite Chern band model analyzed at rs = 10 with self-consistent Hartree-Fock followed by TDHF collective-mode calculations for several values of Berry flux through the first Brillouin zone.
No measurements recorded
Simulatedinfinite Chern band modelStudied Material
Continuum λ-jellium model analyzed with self-consistent Hartree-Fock and TDHF collective-mode calculations, including the effect of varying the Berry curvature scale parameter λ.
No measurements recorded
Simulatedλ-jellium modelStudied Material
Weak periodic potential added as a perturbation to test the robustness of collective-mode topology in the anomalous Hall crystal phase.
No measurements recorded
Simulatedweak periodic potentialStudied Material
Materials
infinite Chern band model
Studied Material
Also known as
infinite Chern band
Variables
model_type= ideal quantum geometry continuum model
model_type= ideal quantum geometry continuum model
studied material
weak periodic potential
Studied Material
Also known as
periodic potentialmoiré periodic potential
Variables
role= perturbation
studied material
Simulations
Workflow
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelinfinite Chern band
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
symmetry breakingcontinuous to discrete translation symmetry imposed by hand
berry flux parameterB A1BZ varied across π/4, 3π/4, 5π/4, 2π
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelλ-jellium
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
lambda parametervaried
Workflow
TDHF calculations with an added weak periodic potential to test robustness of phonon and exciton topology.
model_type= ideal quantum geometry continuum model
studied material
weak periodic potential
Studied Material
Also known as
periodic potentialmoiré periodic potential
Variables
role= perturbation
studied material
Simulations
Workflow
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelinfinite Chern band
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
symmetry breakingcontinuous to discrete translation symmetry imposed by hand
berry flux parameterB A1BZ varied across π/4, 3π/4, 5π/4, 2π
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelλ-jellium
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
lambda parametervaried
Workflow
TDHF calculations with an added weak periodic potential to test robustness of phonon and exciton topology.
model_type= ideal quantum geometry continuum model
studied material
weak periodic potential
Studied Material
Also known as
periodic potentialmoiré periodic potential
Variables
role= perturbation
studied material
Simulations
Workflow
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelinfinite Chern band
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
symmetry breakingcontinuous to discrete translation symmetry imposed by hand
berry flux parameterB A1BZ varied across π/4, 3π/4, 5π/4, 2π
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelλ-jellium
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
lambda parametervaried
Workflow
TDHF calculations with an added weak periodic potential to test robustness of phonon and exciton topology.
model_type= ideal quantum geometry continuum model
studied material
weak periodic potential
Studied Material
Also known as
periodic potentialmoiré periodic potential
Variables
role= perturbation
studied material
Simulations
Workflow
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelinfinite Chern band
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
symmetry breakingcontinuous to discrete translation symmetry imposed by hand
berry flux parameterB A1BZ varied across π/4, 3π/4, 5π/4, 2π
Self-consistent Hartree-Fock followed by time-dependent Hartree-Fock (TDHF) for collective-mode spectra and Chern numbers; band projection to lowest 19 bands on an 18×18 triangular lattice.
Settings
modelλ-jellium
lattice18×18 triangular lattice
bands projected19
collective modesphonons, excitons
lambda parametervaried
Workflow
TDHF calculations with an added weak periodic potential to test robustness of phonon and exciton topology.
Settings
purposetopology robustness check
perturbationweak periodic potential
Conditions
context:periodic-potential perturbation study
Samples:
symmetry breaking
continuous to discrete translation symmetry imposed by hand