Cr2S3-2D is the first single-layer A-type antiferromagnet in which Néel vector switching is observed, enabled by a slight substrate-induced magnetic moment imbalance between its two Cr planes.
Title resolution pending
8 Pith papers cite this work. Polarity classification is still indexing.
8
Pith papers citing it
citation-role summary
method 3
citation-polarity summary
roles
method 3polarities
use method 3representative citing papers
Raman optical activity is observed in ferroaxial NiTiO3 and originates from the ferroaxial order even within the electric dipole approximation.
Strong correlations suppress spin splitting in MnF2 via band narrowing, enable it in MnTe through Mn 3d-Te 5p hybridization, and produce itinerant splitting without local moments in RuO2.
A new equivariant space group framework constructs magnetic Hamiltonians with explicit dependence on magnetic order orientation n, enabling analysis of dynamics-driven topological pumping and ab-initio modeling of real materials.
An end-to-end framework combining domain separation, lightweight ML potentials, and de novo in silico synthesis enables quantitative atomistic modeling of mesoporous metallosilicates that matches experimental densities, pair distribution functions, IR spectra, and hydroxyl densities.
A spin-polarized energy density method derived from spin-density functional theory decomposes total energies into atomic contributions and is implemented in VASP for applications to paramagnetic Fe and Ni-doped GaN.
Sulfur doping in few-layer graphene can preserve linear dispersion, open band gaps of 0.4 eV, induce flat bands at the Fermi level, and cause spin polarization depending on configuration and layer count.
citing papers explorer
-
Strong electron correlations and ligand hybridization for altermagnetism
Strong correlations suppress spin splitting in MnF2 via band narrowing, enable it in MnTe through Mn 3d-Te 5p hybridization, and produce itinerant splitting without local moments in RuO2.
- Collinear ferromagnetism with reduced moment length in kagome magnet Nd3Ru4Al12