For quadratic-band-crossing semimetals, a static sigma-2 mass gives Chern number +-sgn(tx tz), while elliptically polarized light gives Chern number +-sgn(phi); the claimed linear-polarization trivial insulator is actually gapless in the first-order Floquet model.
Anomalous Hall and Nernst effect switching via staggered rotation in a kagome antiferromagnetic semimetal
1 Pith paper cite this work. Polarity classification is still indexing.
abstract
The intricate interplay between magnetism and the topology of electronic structures provides a rich avenue for tailoring materials with unique and potent anomalous transport properties. In this paper, we present a strategy for inducing robust Berry curvature and anomalous transverse conductivity in noncollinear antiferromagnets through an unconventional approach termed ``small \textit{staggered rotation} of spin". Considering noncollinear Mn$_3$Sn, we demonstrate that the positive vector chirality antiferromagnetic configuration, typically associated with a vanishing anomalous Hall effect and Nernst effect, can be manipulated to exhibit finite anomalous Hall conductivity (AHC) and anomalous Nernst conductivity (ANC) through \textit{staggered rotation}. Furthermore, we illustrate that the value and sign of both the AHC and ANC can be tuned through \textit{staggered rotation}. This tuning is intricately influenced by the spin-orbit coupling (SOC) induced gapped nodal line, revealing the critical role of electronic structure modifications in achieving precise control over transport properties.
citation-role summary
citation-polarity summary
fields
cond-mat.mes-hall 1years
2025 1verdicts
CONDITIONAL 1roles
background 1polarities
unclear 1representative citing papers
citing papers explorer
-
Tunable phase transitions from semimetals to Chern insulators in two-dimensional quadratic-band-crossing materials
For quadratic-band-crossing semimetals, a static sigma-2 mass gives Chern number +-sgn(tx tz), while elliptically polarized light gives Chern number +-sgn(phi); the claimed linear-polarization trivial insulator is actually gapless in the first-order Floquet model.