Abstract

Using a first-principles Green's function technique, we study spin-dependent tunneling in two model realizations of (111) fcc $\mathrm{Co}∕{\mathrm{Al}}_{2}{\mathrm{O}}_{3}∕\mathrm{Co}$ tunnel junctions assuming O-terminated crystalline epitaxy in the corundum structure. For the first model, which includes 3 O atoms at the interface, the tunneling current is polarized negatively, just as for the clean Co surface. The second model contains additional oxygen atoms inside large pores at each interface. Located at the three-fold hollow adsorption sites, these O atoms bind very strongly to Co. This bonding creates an interface band in the majority-spin channel which strongly enhances the tunneling current in this channel. As a result, the spin polarization changes sign and becomes positive, similar to that for the oxidized Co surface studied previously. These results show that the common argument of ``mostly $s$-electron tunneling,'' which is often used to explain the positive spin polarization in $\mathrm{Co}∕{\mathrm{Al}}_{2}{\mathrm{O}}_{3}∕\mathrm{Co}$ junctions is quantitatively incorrect. In reality, the spin polarization in these junctions is controlled by the interfacial structure and bonding. Moreover, interfacial adsorption of oxygen may be a prerequisite for achieving the positive spin polarization.

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