A Hall effect variant where magnetic dipoles or ferron-like excitations produce transverse currents.The ferron Hall effect is a variant of the Hall effect where the transverse current is carried by ferrons—quasiparticles that represent collective excitations of magnetic dipoles in a material. Unlike the conventional Hall effect, which involves charged particles, the ferron Hall effect arises from the motion of neutral magnetic excitations, such as magnons or spin waves, that are deflected by a magnetic field or by the material's internal magnetic structure.
The concept of a magnon Hall effect was theoretically proposed in the 2000s and experimentally observed in insulating magnets around 2010. The term 'ferron' is less commonly used, but it refers to the same class of magnetic quasiparticles.
In a magnetic material, the ordered spins can support collective excitations called magnons. When a temperature gradient or an electric field is applied, these magnons can drift, and in the presence of a magnetic field, their trajectories are bent due to the Berry curvature associated with the magnon bands. This deflection creates a transverse heat or spin current, which is the ferron Hall effect. The effect is particularly strong in materials with non-trivial spin textures, such as skyrmions or spin spirals.
It is explored for potential applications in spintronics and magnonics, where heat or spin currents are used for information processing without charge currents.
The ferron Hall effect can occur even in electrically insulating materials, where no charge moves at all, making it a purely magnetic phenomenon.
| v_A | variable | Alfvén wave speed — velocity metre per second |
| B | variable | magnetic field strength — magnetic field strength tesla |
| ρ | variable | mass density — mass density kilogram per cubic metre |
















