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Beilstein J. Nanotechnol. 2018, 9, 2198–2208, doi:10.3762/bjnano.9.206
Figure 1: Specular XRR spectra of CoFeB/IrMn/CoFeB trilayers with tIrMn = 0, 2, 4 and 6 nm.
Figure 2: The field-swept FMR spectra for the sample series recorded at 9 GHz (numbers represent IrMn layer t...
Figure 3: (a) Resonance field Hr as a function of the angle θ at 9 GHz. Open symbols and solid lines represen...
Figure 4: (a) Hr as a function of f for the entire sample series. Open symbols and solid lines represent the ...
Figure 5: (a) ΔH as a function of the frequency with open symbols representing the experimental data and soli...
Figure 6: αeff as a function of the inverse FM layer thickness 1/tCoFeB for different CoFeB/IrMn (2 nm)/CoFeB...
Figure 7: (a) The easy-axis M–H loops of trilayers with varying tIrMn recorded at room temperature (inset sho...
Figure 8: The dependence of (a) Hc and (b) HEB on tIrMn, as extracted from the individual hysteresis loops me...
Figure 9: Two consecutive M–H loops for the trilayer with tIrMn = 4 nm measured at 10 K after field cooling i...