1999
DOI: 10.1016/s0304-8853(99)00346-7
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Mössbauer-effect studies of multilayers and interfaces

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Cited by 100 publications
(52 citation statements)
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“…In M€ ossbauer spectroscopy, the top and the bottom interface of a Fe layer has generally been distinguished by the 57 Fe marker method, 5,14,15 in which case the position of a thin 57 Fe layer (the M€ ossbauer isotope) is varied across the natural Fe layer. The application of this method is limited by the possible mixing and diffusion between the 57 Fe marker and the natural Fe layers, and in case of an extended interface, the quantitative conclusion is difficult.…”
Section: Introductionmentioning
confidence: 99%
“…In M€ ossbauer spectroscopy, the top and the bottom interface of a Fe layer has generally been distinguished by the 57 Fe marker method, 5,14,15 in which case the position of a thin 57 Fe layer (the M€ ossbauer isotope) is varied across the natural Fe layer. The application of this method is limited by the possible mixing and diffusion between the 57 Fe marker and the natural Fe layers, and in case of an extended interface, the quantitative conclusion is difficult.…”
Section: Introductionmentioning
confidence: 99%
“…The spectra in Fig. 1 could be fitted consistently with a Voight-based distribution model [12] of which the mean hyperfine field of 27.2 T matches well with the literature [11]. A Gaussian distribution width σ of 1.2 T is found.…”
Section: Conversion Electron Mössbauer Spectroscopymentioning
confidence: 54%
“…Here, we use the technique to investigate the direction of the c-axis of FePt L1 0 to gain more insight in the crystal growth of FePt L1 0 on MgO(110). For FePt the magnetic moments, and thus the magnetic hyperfine field B hf , are parallel aligned with the c-axis of the tetragonal L1 0 crystal structure [11,3]. The angle θ between the incident gamma-radiation and B hf influences the relative intensities of the lines of a CEMS spectrum.…”
Section: Conversion Electron Mössbauer Spectroscopymentioning
confidence: 99%
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“…Thus, upon annealing, magnetic moments are changing their orientation from in-plane to out-of-plane to random. 38 It may be noted that studied alloy exhibit strong perpendicular magnetic anisotropy in the annealing temperature range of 723 K-923 K (first transformation stage). In the mentioned temperature range, the alloy has peculiar two phase microstructure consisting of FeCo nano-crystals and the remaining amorphous phase, as otherwise, spins are oriented either in-plane or random.…”
Section: Mö Ssbauer Measurementsmentioning
confidence: 99%