“…The exchange bias vanishes above the blocking temperature (T b ), being close to the Neel temperature (T N ) for thick AFM films with large grain sizes, while for thin films T b << T N due to finite size effects [97]. Therefore, the T b value is not characteristic of the material but depends on the AFM thickness [62,97] Through consecutive annealing steps under orthogonal in-plane magnetic fields at different temperatures, the crossed configuration between the magnetization of reference and sensing layers is then defined [62,82,83,98]. The first annealing, performed at higher temperature, sets both AFM fixed layers magnetizations in the same direction, while the second annealing step at a lower temperature sets the soft pinned sensing layer magnetization at a perpendicular direction to the bottom one (Fig.…”