Figure 3
(a) Temperature-dependent resistivity of the single-crystal of YPdBi at a series of magnetic fields H = 0, 1, 2, 3, 4 and 5 T applied fields. (b) Normalized MR as a function of magnetic field H at a series of temperatures T = 5, 50, 100, 200 and 300 K. Here MR = [ρ(H) − ρ(0)]/ρ(0)]× 100%, where ρ(H) and ρ(0) are the resistivity with and without the magnetic field H, respectively. Inset, the observed MR of YPdBi at 300 K (open circles) and fit (black line) with the quadratic equation MR = a|H| + bH2.
