“…Over the past decade, spin–orbit torque (SOT) − has emerged as a promising alternative to spin-transfer torque (STT) and has been intensively investigated. In particular, the SOT-driven switching of ferromagnets (FMs) with perpendicular magnetic anisotropy (PMA) has attracted extensive attention because of its potential for lower-power and faster magnetization manipulations. − , Among various magnetic heterostructures that give rise to PMA, heavy metals (HMs)/CoFeB/MgO becomes standard heterostructures for SOT study ,− because of their compatibility in magnetic tunnel junctions (MTJs) with high tunneling magnetoresistance (TMR). , Usually, HMs with large spin–orbit coupling (SOC) , are the most explored as efficient generators of spin current to produce SOTs, such as Pt, Ir, Ta, W, and some transition metal dichalcogenides . Mo is another 4d transition HM, albeit with a predicted weaker SOC, but it still plays a vital role in the construction of CoFeB/MgO-based perpendicular MTJs (p-MTJs). , …”