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Beilstein J. Nanotechnol. 2022, 13, 1418–1431, doi:10.3762/bjnano.13.117
Figure 1: Geometry of the SF bilayer. We consider the SF interface to be a tunnel barrier. Here, γB is the in...
Figure 2: The evolution of the DOS plotted for increasing values of the exchange field h. Here, γB = 5, df = ...
Figure 3: The evolution of the DOS plotted for increasing values of the SF interface transparency γB. Here, df...
Figure 4: The DOS Nf(E) at the free boundary of the F layer in the SF bilayer in the presence of magnetic and...
Figure 5: The DOS Nf(E) at the free boundary of the F layer in the SF bilayer in the presence of magnetic sca...
Figure 6: The peak at E = Δ in the DOS calculated numerically for three different h (a): h = 1.4Δ (black soli...
Figure 7: The DOS calculated analytically in the limit of low proximity and thin adjacent normal metal layer h...
Figure 8: Current–voltage characteristics of a SFIFS junction in the presence of a spin-dependent scattering....
Figure 9: Comparison of the analytical result in the limit of low proximity and a thin adjacent ferromagnetic...