“…On further decreasing the temperature, this spin splitting and hence the difference in the barrier heights increases. Therefore, the TMR and spin polarization reach the highest values at T = 0 K. The highest value of the spin polarization for the single SF junction can reach 77%, which is qualitatively in agreement with the experimental measurements [7] and the theoretical results [24,25], while for the double SF junction (in the parallel alignment), it approaches 66% for c = 0.50 nm and 99% for c = 0.72 nm [18], which is due to the change in the positions of the spin-polarized quasibound states in the quantum well. Therefore, one can see that, for the double SF junctions, the TMR and the spin polarization of the tunnelling current can be controlled by the thickness of the central NM layer, the temperature and the applied bias.…”