IrMn blocking temperature (T-B) is compared between IrMn/Co bilayers and (Pt/Co)(3)/IrMn/Co and (Pd/Co)(3)/IrMn/Co trilayers for different IrMn thicknesses. Exchange bias field (H-ex) is measured from 5 to 400 K. Trilayers show a more concave thermal decrease of H-ex(T) compared to bilayers and, for thin IrMn layers, larger T-B and sharper peak of coercive field H-c around T-B. This H-ex(T) behaviour presents improved characteristics for thermally assisted-MRAM (TA-MRAM) applications, with large H-ex/H-c ratio. Two physical explanations are proposed: an indirect IrMn intergrain coupling through the (Pt(Pd)/Co)(3) layer and a reduction of IrMn/Co interfacial coupling due to out-of-plane canting of the IrMn spins.

Enhanced blocking temperature in (Pt/Co)(3)/IrMn/Co and (Pd/Co)(3)/IrMn/Co trilayers with ultrathin IrMn layer

Vinai G;
2013

Abstract

IrMn blocking temperature (T-B) is compared between IrMn/Co bilayers and (Pt/Co)(3)/IrMn/Co and (Pd/Co)(3)/IrMn/Co trilayers for different IrMn thicknesses. Exchange bias field (H-ex) is measured from 5 to 400 K. Trilayers show a more concave thermal decrease of H-ex(T) compared to bilayers and, for thin IrMn layers, larger T-B and sharper peak of coercive field H-c around T-B. This H-ex(T) behaviour presents improved characteristics for thermally assisted-MRAM (TA-MRAM) applications, with large H-ex/H-c ratio. Two physical explanations are proposed: an indirect IrMn intergrain coupling through the (Pt(Pd)/Co)(3) layer and a reduction of IrMn/Co interfacial coupling due to out-of-plane canting of the IrMn spins.
2013
exchange bias
magnetism
interface coupling
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/350541
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