Anomalous Hall Effect due to the spin chirality in the Kagomé lattice

In order to do so, compare the free energy of a perfectly ordered system with the free energy of a partially disordered case that introduces the less energetic frustrations

Namely: the effect of the effective magnetic field due to spin- orbit scattering, the electric charge accumulation with electrostatic interactions and screening, and the

Before presenting the example of an electrically isotropic composite having a negative Hall coef- ficient even though it is built from three phases each having a positive

S’il s’agit de passer de l’orbite ext´ erieure ` a l’orbite int´ erieure, il suffit d’appliquer un d´ ecr´ ement de vitesse ∆v B au point B (i.e. d’utiliser des

at high temperatures TCNQ carriers are electron-like and HMTSeF carriers are hole-like, thus a larger mobility of the HMTSeF electrons may account for the sign of

When an external field is applied to a sample in the normal Hall geometry there is a net alignment of the moments and the asymmetric scattering events combine to produce an

i j In performing the subsequent Anergy inte- grations, we use the fact thaz BE^>>^ to approximate the integrals by their (exponentially large) maximum multiplied by

The main properties of this inner magnetospheric region are briefly recalled. The dynamical response of the plasma s phere to enhancements of geomagnetic activity