The intrinsic Berry curvature in ferromagnetic (FM) materials significantly influences Hall conductivity during the antiferromagnetic (AFM)-to-FM phase transition, as demonstrated through the anomalous Hall effect (AHE). First-principles calculations indicate negligible spin Hall conductivity in FeRh materials in the AFM phase due to time-reversal symmetry breaking. To date, the contribution of the Berry curvature to the spin Hall effect remains unexamined in the context of AHE measurements. This study presents the temperature-dependent spin and carrier transport properties of FeRh thin films across AFM-to-FM transitions. In the AFM phase, a nonzero AHE signal is observed and even reverses its sign when the film transitions to the FM phase (above