2014
DOI: 10.1063/1.4865569
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Enhancement of the magnetic interfacial exchange energy at a specific interface in NiFe/CoO/Co trilayer thin films via ion-beam modification

Abstract: Enhancement of the magnetic interfacial exchange energy at a specific interface Enhancement of the magnetic interfacial exchange energy at a specific interface in NiFe/CoO/Co trilayer thin films via ion-beam modification in NiFe/CoO/Co trilayer thin films via ion-beam modification

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Cited by 16 publications
(8 citation statements)
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“…1 f), we observe a qualitative transition in the shape of the MOKE hysteresis loop. While measurements conducted with relatively low pump fluence produce transient signals with sharp switching features, measurements taken at high pump fluences instead display two-step magnetization switching, suggesting different regions of the sample experience distinct coercive fields 27 , 28 . In the two-step hysteresis loops it is salient that one part narrows sharply, displaying a dramatically reduced coercivity of 33 Oe, while the remaining switching signal is comparatively resilient with a saturation field of approximately 430 Oe.…”
Section: Resultsmentioning
confidence: 97%
“…1 f), we observe a qualitative transition in the shape of the MOKE hysteresis loop. While measurements conducted with relatively low pump fluence produce transient signals with sharp switching features, measurements taken at high pump fluences instead display two-step magnetization switching, suggesting different regions of the sample experience distinct coercive fields 27 , 28 . In the two-step hysteresis loops it is salient that one part narrows sharply, displaying a dramatically reduced coercivity of 33 Oe, while the remaining switching signal is comparatively resilient with a saturation field of approximately 430 Oe.…”
Section: Resultsmentioning
confidence: 97%
“…While measurements conducted with relatively low pump uence produce transient signals with sharp switching features, measurements taken at high pump uences instead display two-step magnetization switching, suggesting different regions of the sample experience distinct coercive elds. [23,24] In the two-step hysteresis loops it is salient that one part narrows sharply, displaying a dramatically reduced coercivity of 33 Oe, while the remaining switching signal is comparatively resilient with a saturation eld of approximately 430 Oe. Such a dynamical magnetic structure is analogous to a spin-valve-like "hard-soft" bilayer set.…”
Section: Resultsmentioning
confidence: 99%
“…The structural depth profile of the layered sample is encoded in the reflectivity as a function of the scattering vector Q. PNR experiments were performed on the time-of-flight PLATYPUS reflectometer at the OPAL Research Reactor, Australia. 15,21,[29][30][31] The PNR samples were field-cooled in 10 kOe from 310 K to 110 K, and the spin-dependent neutron reflectivity channels R + and R − were measured at 110 K and upon warming to 310 K. The difference between the R + and R − reflectivity channels gives the spin asymmetry SA = (R + − R − )/(R + + R − ) of a sample as a function of the scattering vector Q. The depth-dependence of the sample's in-plane magnetic moment is encoded in the Q-dependence of the SA data.…”
Section: Experimental Methodsmentioning
confidence: 99%