Abstract

The structure of Fe films, epitaxially grown on Ni(001), has been studied in the 0--14 ML coverage range by means of photoelectron diffraction (PD) in the forward scattering regime. Quantitative analysis by a multiple scattering approach has been performed on Fe films at a coverage of 3 and 7 ML. Analysis of the 3-ML data showed that growth was not layer-by-layer but rather occurred through islands nucleation and that transition from the pseudomorphic fcc to the bcc phase was located in this early stage of growth. In fact, best fit was obtained by calculations on a 2 ML bcc(110)/3 ML fcc(001) Fe film with the $\mathrm{bcc}〈111〉\ensuremath{\parallel}\mathrm{fcc}〈110〉$ in-plane orientation. Interlayer spacings of $2.05\ifmmode\pm\else\textpm\fi{}0.06\AA{},$ $2.01\ifmmode\pm\else\textpm\fi{}0.03\AA{},$ and $1.85\ifmmode\pm\else\textpm\fi{}0.03\AA{}$ were found in the bcc region, between bcc and fcc layers and in the fcc region, respectively. Best-fit in-plane nearest-neighbors (n-n) distance was $2.49\ifmmode\pm\else\textpm\fi{}0.02\AA{},$ in registry with that of the Ni substrate. To analyze the 7-ML data a 4 ML bcc(110)/3 ML fcc(001) film was employed, varying the fitting parameters in the bcc region only. Best fit was obtained for an interlayer spacing of $2.04\ifmmode\pm\else\textpm\fi{}0.04\AA{}$ and in plane n-n distance of $2.47\ifmmode\pm\else\textpm\fi{}0.01\AA{}.$ At 14 ML the PD pattern collected over a 94\ifmmode^\circ\else\textdegree\fi{} azimuthal range displayed symmetry around the [110] substrate direction, which was explained by the equipopulation of the 4 bcc(110) domains satisfying the $\mathrm{bcc}〈111〉\ensuremath{\parallel}\mathrm{fcc}〈110〉$ alignment.

Highlights

  • The face centered cubicfccphase of Fe␥-Feat low temperature has been the subject of many theoretical and experimental investigations due to the strong dependence of its magnetic properties on the atomic volume: the so-called magneto-volume instability.[1,2,3,4,5] As ␥-Fe is stable in bulk phase only above 910 °C, epitaxial growth of thin-Fe films on suitable fcc substrates is needed to stabilize it at room temperatureRT

  • Quantitative analysis by a multiple scattering approach has been performed on Fe films at a coverage of 3 and 7 ML

  • Best fit was obtained by calculations on a 2 ML bcc110͒/3 ML fcc001͒ Fe film with the bcc111͘ʈfcc110͘ in-plane orientation

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Summary

Introduction

The face centered cubicfccphase of Fe␥-Feat low temperature has been the subject of many theoretical and experimental investigations due to the strong dependence of its magnetic properties on the atomic volume: the so-called magneto-volume instability.[1,2,3,4,5] As ␥-Fe is stable in bulk phase only above 910 °C, epitaxial growth of thin-Fe films on suitable fcc substrates is needed to stabilize it at room temperatureRT In this way, by forcing a pseudomorphic growth and playing with the value of the substrate lattice constant it is possible to tailor the Fe atomic volume in the growing film. Ni is suitable, its lattice constant being 3.52 ÅϪ2% lattice mismatch, and both theoretical and experimental studies have confirmed the influence of the substrate magnetism on the Fe overlayer.[7,8]

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