Non-collinear magnetization structure at the thickness and
Transkrypt
Non-collinear magnetization structure at the thickness and
Non-collinear magnetization structure at the thickness and temperature driven spin reorientation transition in ultrathin epitaxial Fe films on W(110) Ślęzak T.1, Ślęzak M.1, Kozioł-Rachwał A.1, Matlak K.1, Freindl K. 3, Spiridis N. 3, E. PartykaJankowska4, D. Wilgocka-Ślęzak3, Zając M. 1,2, Rüffer R.2, Korecki J.1,3 1 Faculty of Physics and Applied Computer Science, AGH, Kraków, Poland European Synchrotron Radiation Facility, BP 220, 38043 Grenoble Cedex, France 3 Institute of Catalysis and Surface Chemistry, PAN, ul. Niezapominajek 8, Kraków, Poland 4 Faculty of Physics, University of Vienna, A-1090 Wien, Austria 2 Thickness and temperature induced in-plane spin reorientation transition (SRT) in epitaxial Fe films on W(110) [1] was studied in situ using the nuclear resonant scattering of synchrotron radiation. NRS is a synchrotron analogue of Mössbauer spectroscopy (MS), in the sense that recoilless excitation (induced by the resonant x-rays with energy 14.4 keV for 57Fe) of the nuclear energy levels, split due to the hyperfine interactions, is involved [2]. In this method, the hyperfine parameters can be obtained from a characteristic beat pattern seen in the time evolution of the intensity of nuclear resonant scattering (the so called time spectrum). The well defined polarization of the synchrotron x-rays provides high sensitivity to the orientation of the hyperfine magnetic field and electric field gradient. The numerical analysis of the NRS time spectra measured during Fe evaporation, indicates that transition from the uniform [1-10] oriented magnetization state observed at lower thickness to the [001] magnetization orientation at higher thickness undergoes via formation of non-collinear spin structure. It is clear that with increasing film thickness the bottom Fe(110) atomic layers initiate SRT while the surface magnetization reverses at the end. This thickness induced SRT originates at the Fe/W(110) interface and proceeds via a non-collinear spin structure resembling a planar domain wall that propagates towards the surface with increasing film thickness. It was shown that thickness induced SRT process at 250°C proceeds also trough the intermediate, vertically non-collinear magnetic state but in contrast to the room temperature thickness driven reorientation the spin spiral state has opposite sense of rotation namely: with increasing thickness magnetization reorientation from [1-10] to [001] direction is initiated by the top most atomic layers and completed at the Fe/W(110) interface. The nature of the temperature induced transition is also non-collinear and with increasing temperature surface magnetization switches first from [1-10] to [001] direction. [1] Gradmann U., Korecki J., Waller C., Appl. Phys. A 39 101 (1986) [2] Sturhahn W., Hyperfine Interact. 125, 149 (2000) This work was supported by the Team Program of the Foundation for Polish Science cofinanced by the EU European Regional Development Fund.