2020
DOI: 10.1107/s2052520620005727
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Prediction of orientation relationships and interface structures between α-, β-, γ-FeSi2 and Si phases

Abstract: A pure crystallogeometrical approach is proposed for predicting orientation relationships, habit planes and atomic structures of the interfaces between phases, which is applicable to systems of low-symmetry phases and epitaxial thin film growth. The suggested models are verified with the example of epitaxial growth of -,and -FeSi 2 silicide thin films on silicon substrates. The density of near-coincidence sites is shown to have a decisive role in the determination of epitaxial thin film orientation and explain… Show more

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Cited by 7 publications
(3 citation statements)
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“…According to the interpretation of the diffraction pattern [ 31 ], the epi-layer has the following OR: Fe 3+ x Si 1− x (111) [0−11]||Si(111) [1−10]. The strain [ 33 ] is 3.54%, and the area misfit is −8.35% for this epitaxial OR. Thus, the c lattice parameter is under the same compressive stress while the a and b parameters are slightly relaxed.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…According to the interpretation of the diffraction pattern [ 31 ], the epi-layer has the following OR: Fe 3+ x Si 1− x (111) [0−11]||Si(111) [1−10]. The strain [ 33 ] is 3.54%, and the area misfit is −8.35% for this epitaxial OR. Thus, the c lattice parameter is under the same compressive stress while the a and b parameters are slightly relaxed.…”
Section: Resultsmentioning
confidence: 99%
“…The 2D dislocation lattice presented in Figure 9 b was constructed by overlapping two lattices of stoichiometric Fe 3 Si and silicon with the experimental OR [ 43 ]. Figure 9 b also shows the distribution of near coincidence sites on the interface of stoichiometric iron silicide [ 33 , 44 ]. The structural motif of the spatial distribution of the dislocation borders can be easily observed on the dark field images by the TEM technique in over-focus mode measured in plan view for the one 40 nm thick Fe 3+ x Si 1− x layer grown on Si(111) with the same procedure described above.…”
Section: Resultsmentioning
confidence: 99%
“…The reason for the occurrence of additional states at 20 meV could be an interlayer of another Fe-Si phase at the β-FeSi 2 /Si interface. For the growth of β-FeSi 2 on Si surfaces it was experimentally observed [3] and theoretically described [77,88] that the interface energy between the two components, having a rather large lattice mismatch, can be reduced by an α-FeSi 2 interlayer. Furthermore, the z-polarized PDOS of α-FeSi 2 exhibits a distinct peak at 20 meV [86].…”
Section: B Lattice Dynamicsmentioning
confidence: 96%