2016
DOI: 10.1063/1.4944405
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Magnetic and structural properties of MnRh thin films

Abstract: Enhanced saturation magnetization in perpendicular L1 0 -MnAl films upon low substitution of Mn by 3d transition metals

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Cited by 3 publications
(3 citation statements)
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“…The effect of such interfacial magnetic frustration also increases with decreasing the layer thickness t and could significantly contribute together with strain to the suppression of metamagnetism in FeRh. 60 Assuming that the MnRh layers are always in the FM phase, we calculated the fraction of the residual FM phase in the FeRh layers at low temperatures, assuming a MnRh saturation magnetization of 120 kA/m at 70 K. 49 While the t = 3 nm superlattice remains FM at all temperatures, all superlattices with a larger t feature a residual FM fraction, which decreases with the increasing individual layer thickness (see Table 2). The residual FM FeRh fraction is likely distributed across all FeRh layers in the stack, located at the interface and surface regions of the constituent films.…”
Section: Methodsmentioning
confidence: 79%
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“…The effect of such interfacial magnetic frustration also increases with decreasing the layer thickness t and could significantly contribute together with strain to the suppression of metamagnetism in FeRh. 60 Assuming that the MnRh layers are always in the FM phase, we calculated the fraction of the residual FM phase in the FeRh layers at low temperatures, assuming a MnRh saturation magnetization of 120 kA/m at 70 K. 49 While the t = 3 nm superlattice remains FM at all temperatures, all superlattices with a larger t feature a residual FM fraction, which decreases with the increasing individual layer thickness (see Table 2). The residual FM FeRh fraction is likely distributed across all FeRh layers in the stack, located at the interface and surface regions of the constituent films.…”
Section: Methodsmentioning
confidence: 79%
“…Assuming that the MnRh layers are always in the FM phase, we calculated the fraction of the residual FM phase in the FeRh layers at low temperatures, assuming a MnRh saturation magnetization of 120 kA/m at 70 K . While the t = 3 nm superlattice remains FM at all temperatures, all superlattices with a larger t feature a residual FM fraction, which decreases with the increasing individual layer thickness (see Table ).…”
Section: Resultsmentioning
confidence: 99%
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