The large magnetic anisotropy in the layered ferromagnet Fe_{ 1/4}TaS_2 leads to very sharp reversals of the magnetization $\bf M$ at the coercive field. We have exploited this feature to measure the anomalous Hall effect (AHE), focussing on the AHE conductivity $\sigma^A_{ xy}$ in the inelastic regime. At low temperature T (5-50 K), $\sigma^A_{ xy}$ is T-independent, consistent with the Berry-phase/Karplus-Luttinger theory. Above 50 K, we extract an inelastic AHE conductivity $\sigma^{ in}_{ xy}$ that scales as the square of $\Delta\rho$ (the T dependent part of the resistivity $\rho$). The term $\sigma^{ in}_{ xy}$ clarifies the T dependence and sign-reversal of the AHE coefficient R_s(T). We discuss the possible ubiquity of $\sigma^{ in}_{ xy}$ in ferromagnets, and ideas for interpreting its scaling with $(\Delta\rho)^2$. Measurements of the magnetoresistance (MR) reveal a rich pattern of behavior vs. T and field tilt-angle. We show that the 2 mechanisms, the anisotropic MR effect and field-suppression of magnons, account for the intricate MR behavior, including the bow-tie features caused by the sharp reversals in $\bf M$.
Categories: cond-mat.str-el cond-mat.mes-hall