as a function of film thickness and temperature. The intrinsic contribution from the Berry
curvature is singled out from the extrinsic ones and determined to be 821 Ω− 1 cm− 1, which
agrees to the theoretical prediction of 842 Ω− 1 cm− 1 and is considerably smaller than 1100
Ω− 1 cm− 1 for Fe (001). This result provides a direct experimental evidence for the
anisotropy of the intrinsic AHE in single crystal Fe, reflecting its electronic band structure.