Abstract

The growth and magnetic properties of thin Fe films deposited at room temperature on ultrathin iron silicide seed layer epitaxially grown on Si(111) single crystal were investigated as a function of Fe thickness ($0<{t}_{\mathrm{Fe}}<300$ monolayers). The growth mode and structure have been determined in situ by means of scanning tunneling microscopy, low energy electron diffraction, and x-ray photoelectron diffraction. The magnetic properties were characterized ex situ by conventional polar and longitudinal magneto-optical Kerr effect, transverse biased initial inverse susceptibility and torque (TBIIST) measurements, and superconducting quantum interference device magnetometry. Fe growth is of Volmer-Weber type (island growth) and the epitaxial film adopts the bcc $\ensuremath{\alpha}$-Fe structure. Onset of long-range ferromagnetic order occurs at 4.7 monolayers (ML), in the vicinity of the percolation threshold of the Fe islands. The Curie temperature increases continuously with Fe coverage, varying from 135 K for 4.7 ML to 260 K for 7.3 ML. Two different spin reorientation transitions have been observed versus Fe coverage. First, the magnetic easy axis rotates from normal to the film plane, for coverage below 6 ML, to in plane, for thickness above 7 ML. Then, in-plane magnetized films present tiny (anisotropy fields less than 4 Oe) uniaxial and sixfold magnetic anisotropies. From sixfold anisotropy the small higher order cubic anisotropy constant ${K}_{2}$ was measured precisely by TBIIST. It decreases monotonously with increasing coverage and changes its sign at approximately 20 ML, which in turn results in a switching of the sixfold anisotropy easy axis from ⟨1--10⟩ to ⟨1--21⟩ directions. It appears that TIBIIST magnetometry is a powerful method for a quantitative determination of the various contributions to in-plane magnetic anisotropies in ultrathin films.

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