Anisotropic magnetotransport realized in doped hematite

Conventional antiferromagnetic materials have long been recognized for their time-reversal symmetry, resulting in a zero anomalous Hall coefficient. However, a paradigm shift occurs when examining easy-axis antiferromagnets and their spin-flop transition. This transition introduces a magnetic canted moment, leading to the emergence of a non-zero anomalous Hall signal and the generation of a non-dissipative transversal current. While high symmetry systems typically manifest an isotropic Hall effect, our study unveils the extraordinary behavior exhibited by hematite that becomes conductive due to small Ti doping. We investigate the magnetotransport in Titanium-doped hematite, uncovering a highly pronounced and unconventional symmetry. Notably, this effect displays a remarkable dependence on the crystal orientation of the material. We establish a compelling correlation between our experimental observations and the predicted anomalous Hall effect in altermagnets through symmetry analysis. This study expands our understanding of the Hall effect in antiferromagnetic materials and sheds light on the intricate interplay between crystal orientation and unconventional Hall phenomena.