“…The multiband nature of EuGa 4 is clearly evident from the nonlinear behavior of ρ x y (H) [see e.g., ρ x y (H) at 20 K in figure 5(f)], as confirmed also by de Haas-van Alphen (dHvA) studies and by electronic band-structure calculations [48,49,52]. Similar to BaAl 4 and EuAl 4 [44,46,47], at high temperatures, the ρ x y (H) of EuGa 4 is dominated by the holes while, at low temperatures, mostly the electrons account for the Hall signal. In the AFM state [see figures 5(a)-(d)], a hump-like anomaly in the ρ x y (H) gradually develops with decreasing temperature, reminiscent of the topological Hall resistivity arising from topological spin textures [3,17,19,21,23,24,25,26,27,28,29,31].…”