2005
DOI: 10.1063/1.1855011
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Growth, structure, and magnetism of γ-phase Mn ultrathin films on Cu3Au(100)

Abstract: Ultrathin γ-phase (face-center cubic) Mn films were prepared by epitaxial growth on Cu3Au(100). Kinematic analysis of low energy electron diffraction I∕V showed a structure transformation of Mn films from nearly face-center cubic to face-center tetragonal with increasing coverage. No ferromagnetic signal in Mn∕Cu3Au(100) was observed. For 21 ML capping film of Fe on Mn films, the hysteresis loop of Fe was biased. The bias field for 21MLFe∕15MLMn∕Cu3Au(100) was ∼200Oe at 110 K with the blocking temperature Tb∼3… Show more

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Cited by 5 publications
(2 citation statements)
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“…[29] However, this was not the case for all growth conditions. [27,[30][31][32][33] In our case, MEED oscillations for the growth of Mn=Cu 3 Auð001Þ up to thicknesses above 60 ML could be observed. [34] An oscillating MEED intensity, which is a fingerprint of a layer-by-layer growth mode, was found for all disordered Ni x Mn 100Àx alloys and the ALF.…”
Section: Resultsmentioning
confidence: 94%
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“…[29] However, this was not the case for all growth conditions. [27,[30][31][32][33] In our case, MEED oscillations for the growth of Mn=Cu 3 Auð001Þ up to thicknesses above 60 ML could be observed. [34] An oscillating MEED intensity, which is a fingerprint of a layer-by-layer growth mode, was found for all disordered Ni x Mn 100Àx alloys and the ALF.…”
Section: Resultsmentioning
confidence: 94%
“…Its presence in disordered Ni x Mn 100Àx alloy films and pure Mn films on Cu 3 Auð001Þ has been discussed before. [25,30,31] The layer-by-layer growth opens the way to atomic-scale manipulation of the interface roughness. [42] In the present study, we have stopped the growth of the Ni and Mn layers at the maxima of the specularly reflected (00)-spot MEED intensity, minimizing the roughness.…”
Section: Resultsmentioning
confidence: 99%