“…Recently, antiferromagnetically coupled materials, such as ferrimagnets, synthetic antiferromagnets (AFMs), and AFMs, have attracted significant attention due to their promising potential in spintronic applications because of several properties, such as the absence of stray magnetic fields, terahertz spin dynamics, and stability against external perturbations [5][6][7] . The electrical current switching of the AFM Néel vector has been demonstrated for several AFM materials, such as CuMnAs 8,9 , Mn 2 Au 10,11 , NiO [12][13][14] , and Fe 2 O 3 15 , with electrical current densities on the order of 10 7 -10 8 A/cm 2 , and recently switching with the order of 10 6 A/cm 2 has been realized on noncollinear AFM of Mn 3 GaN 16 and Mn 3 Sn 17 . In addition, the electrical current switching of ferrimagnets has been demonstrated.…”