Figure 2. Chiral anomaly induced negative longitudinal MR in sample N1.
(a) MR in three different geometries in transport measurements at 2.5 K. (b) The negative MR only appears when E is parallel with B. The control experiments with geometries II and III exclude the crystal anisotropy effect on the observed negative MR. (c) The magneto-conductance change σB–σ0 at different temperatures, following a quadratic dependence, and it decreases after a critical field. The inset summarizes the fitting coefficient α at different temperatures.