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Asymmetric Interfaces in Epitaxial Off-Stoichiometric Fe(3+x)Si(1−x)/Ge/Fe(3+x)Si(1−x) Hybrid Structures: Effect on Magnetic and Electric Transport Properties

Three-layer iron-rich Fe(3+x)Si(1−x)/Ge/Fe(3+x)Si(1−x) (0.2 < x < 0.64) heterostructures on a Si(111) surface with Ge thicknesses of 4 nm and 7 nm were grown by molecular beam epitaxy. Systematic studies of the structural and morphological properties of the synthesized samples have shown that...

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Detalles Bibliográficos
Autores principales: Tarasov, Anton S., Tarasov, Ivan A., Yakovlev, Ivan A., Rautskii, Mikhail V., Bondarev, Ilya A., Lukyanenko, Anna V., Platunov, Mikhail S., Volochaev, Mikhail N., Efimov, Dmitriy D., Goikhman, Aleksandr Yu., Belyaev, Boris A., Baron, Filipp A., Shanidze, Lev V., Farle, Michael, Varnakov, Sergey N., Ovchinnikov, Sergei G., Volkov, Nikita V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8747018/
https://www.ncbi.nlm.nih.gov/pubmed/35010081
http://dx.doi.org/10.3390/nano12010131
Descripción
Sumario:Three-layer iron-rich Fe(3+x)Si(1−x)/Ge/Fe(3+x)Si(1−x) (0.2 < x < 0.64) heterostructures on a Si(111) surface with Ge thicknesses of 4 nm and 7 nm were grown by molecular beam epitaxy. Systematic studies of the structural and morphological properties of the synthesized samples have shown that an increase in the Ge thickness causes a prolonged atomic diffusion through the interfaces, which significantly increases the lattice misfits in the Ge/Fe(3+x)Si(1−x) heterosystem due to the incorporation of Ge atoms into the Fe(3+x)Si(1−x) bottom layer. The resultant lowering of the total free energy caused by the development of the surface roughness results in a transition from an epitaxial to a polycrystalline growth of the upper Fe(3+x)Si(1−x). The average lattice distortion and residual stress of the upper Fe(3+x)Si(1−x) were determined by electron diffraction and theoretical calculations to be equivalent to 0.2 GPa for the upper epitaxial layer with a volume misfit of −0.63% compared with a undistorted counterpart. The volume misfit follows the resultant interatomic misfit of |0.42|% with the bottom Ge layer, independently determined by atomic force microscopy. The variation in structural order and morphology significantly changes the magnetic properties of the upper Fe(3+x)Si(1−x) layer and leads to a subtle effect on the transport properties of the Ge layer. Both hysteresis loops and FMR spectra differ for the structures with 4 nm and 7 nm Ge layers. The FMR spectra exhibit two distinct absorption lines corresponding to two layers of ferromagnetic Fe(3+x)Si(1−x) films. At the same time, a third FMR line appears in the sample with the thicker Ge. The angular dependences of the resonance field of the FMR spectra measured in the plane of the film have a pronounced easy-axis type anisotropy, as well as an anisotropy corresponding to the cubic crystal symmetry of Fe(3+x)Si(1−x), which implies the epitaxial orientation relationship of Fe(3+x)Si(1−x) (111)[0−11] || Ge(111)[1−10] || Fe(3+x)Si(1−x) (111)[0−11] || Si(111)[1−10]. Calculated from ferromagnetic resonance (FMR) data saturation magnetization exceeds 1000 kA/m. The temperature dependence of the electrical resistivity of a Ge layer with thicknesses of 4 nm and 7 nm is of semiconducting type, which is, however, determined by different transport mechanisms.