Ellipsometer Mounting System Design Using CAD

Рассматривается задача автоматизированного проектирования системы крепления плеч эллип- сометра, являющегося частью установки молекулярно-лучевой эпитаксии с магнитооптическим эллипсометрическим комплексом. Показана возможность проектирования, управляемого задан- ными ограничивающими условиями. При помощи системы автоматизированного проектирова- ния с использованием математического моделирования была найдена оптимальная форма креп- ления плеч эллипсометра. Было определено ускорение, возникающее при типичных перегрузках камеры, при этом максимальное отклонение луча на приемнике анализатора не превышало до- пустимого для проведения измерений отклонения.Ellipsometer arms mounting is a part of MBE system with magneto-optic ellipsometric complex, for which the automated designing task has been examined. The ability of the limiting conditions driven design has been shown. Using CAD and mathematical modeling the optimal form of ellipsometer mounting arms was found. The acceleration that appears under typical mechanical overloads has been defined, under the condition that the maximum beam deviation of the analyzer did not exceed the admissible deviation for carrying out measurements

Ellipsometer Mounting System Design Using CAD

Рассматривается задача автоматизированного проектирования системы крепления плеч эллип- сометра, являющегося частью установки молекулярно-лучевой эпитаксии с магнитооптическим эллипсометрическим комплексом. Показана возможность проектирования, управляемого задан- ными ограничивающими условиями. При помощи системы автоматизированного проектирова- ния с использованием математического моделирования была найдена оптимальная форма креп- ления плеч эллипсометра. Было определено ускорение, возникающее при типичных перегрузках камеры, при этом максимальное отклонение луча на приемнике анализатора не превышало до- пустимого для проведения измерений отклонения.Ellipsometer arms mounting is a part of MBE system with magneto-optic ellipsometric complex, for which the automated designing task has been examined. The ability of the limiting conditions driven design has been shown. Using CAD and mathematical modeling the optimal form of ellipsometer mounting arms was found. The acceleration that appears under typical mechanical overloads has been defined, under the condition that the maximum beam deviation of the analyzer did not exceed the admissible deviation for carrying out measurements

Growth Process, Structure and Electronic Properties of Cr₂GeC and Cr_2-xMn_xGeC Thin Films Prepared by Magnetron Sputtering

The growth and phase formation features, along with the influence of structure and morphology on the electronic, optical, and transport properties of Cr2GeC and Cr2-xMnxGeC MAX phase thin films synthesized by magnetron sputtering technique, were studied. It was found that the Cr:Ge:C atomic ratios most likely play the main role in the formation of a thin film of the MAX phase. A slight excess of carbon and manganese doping significantly improved the phase composition of the films. Cr2GeC films with a thicknesses exceeding 40 nm consisted of crystallites with well-developed facets, exhibiting metallic optical and transport properties. The hopping conduction observed in the Cr2-xMnxGeC film could be attributed to the columnar form of crystallites. Calculations based on a two-band model indicated high carrier concentrations N, P and mobility μ in the best-synthesized Cr2GeC film, suggesting transport properties close to single crystal material. The findings of this study can be utilized to enhance the growth technology of MAX phase thin films

Substitution Effects in Spin-Polarized (Cr_4-xFe_x)_0.5AC (A = Ge, Si, Al) MAX Phases

The use of spintronic devices with a tunable magnetic order on small scales is highly important for novel applications. The MAX phases containing transition metals and/or magnetic ion-substituted lattices attract a lot of attention. In this study, the magnetic and electronic properties of (Cr4-xFex)0.5AC (A = Ge, Si, Al) compounds were predicted and investigated within the density functional theory. It was established that single-substituted (Cr3Fe1)0.5AC (A = Ge, Si, Al) lattices are favorable in terms of energy. An analysis of the magnetic states of the MAX phases demonstrated that their spin order changes upon substitution of iron atoms for chromium ones. It was found that mostly the (Cr4-xFex)0.5GeC and (Cr4-xFex)0.5AlC lattices acquire a ferrimagnetic state in contrast to (Cr4-xFex)0.5SiC for which the ferromagnetic spin order dominates. It was pointed out that the atomic substitution could be an efficient way to tune the magnetic properties of proposed (Cr4-xFex)0.5AC (A = Ge, Si, Al) MAX phases

Asymmetric Interfaces in Epitaxial Off-Stoichiometric Fe3+xSi1−x/Ge/Fe3+xSi1−x Hybrid Structures: Effect on Magnetic and Electric Transport Properties

Three-layer iron-rich Fe3+xSi1−x/Ge/Fe3+xSi1−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/Fe3+xSi1−x heterosystem due to the incorporation of Ge atoms into the Fe3+xSi1−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 Fe3+xSi1−x. The average lattice distortion and residual stress of the upper Fe3+xSi1−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 Fe3+xSi1−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 Fe3+xSi1−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 Fe3+xSi1−x, which implies the epitaxial orientation relationship of Fe3+xSi1−x (111)[0−11] || Ge(111)[1−10] || Fe3+xSi1−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