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The exchange-coupled [Co/Ni]N/Tb Fe nano-magnetic films can display strong perpendicular magnetic anisotropy(PMA) which depends on the Tb:Fe component ratio, Tb Fe layer thickness and the repetition number N of [Co/Ni]Nmultilayer. Perpendicular spin valves in the nano thickness scale, consisting of a [Co/Ni]3free and a [Co/Ni]5/Tb Fe reference multilayer, show high giant magnetoresistance(GMR) signal of 6.5 % and a large switching field difference over3 k Oe. However, unexpected slanting of the free layer magnetization, accompanied by a reduced GMR ratio, was found to be caused by the presence of a thick Fe-rich or even a thin but Tb-rich Tb Fe layer. We attribute this phenomenon to the large magnetostriction effect of Tb Fe which probably induces strong stress acting on the free layer and hence reduces its interfacial PMA.
The exchange-coupled [Co / Ni] N / Tb Fe nano-magnetic films can display strong perpendicular magnetic anisotropy (PMA) which depends on the Tb: Fe component ratio, Tb Fe layer thickness and the repetition number N of [Co / Ni ] Nmultilayer. Perpendicular spin valves in the nano thickness scale, consisting of a [Co / Ni] 3 free and a [Co / Ni] 5 / Tb Fe reference multilayer, show high giant magnetoresistance (GMR) signal of 6.5% and a large switching However, unexpected slanting of the free layer magnetization, accompanied by a reduced GMR ratio, was found to be caused by the presence of a thick Fe-rich or even a thin but Tb-rich Tb Fe layer. We attribute this phenomenon to the large magnetostriction effect of Tb Fe which probably induces strong stress acting on the free layer and subsequently to its interfacial PMA.