Fig. 4: Odd-in-magnetic field component of the angular-dependent transverse magnetoresistance due to anomalous Hall effect.
a, b Odd contributions to ρ⊥,x and ρ⊥,y obtained after subtraction of the dominating even-in-field contribution from raw data at 2 T shown in Fig. 2c, d. The even-in-field contribution was determined by fitting \({\sum }_{n = 2,4,6,8,10}{A}_{n}\cos (n\alpha +{\alpha }_{n})\). The odd component is dominated by a threefold symmetry which is highlighted by the continuous line representing a guide to the eye proportional to \({A}_{3}\cos (3\alpha +{\alpha }_{3})\).
