Engineering Papers⌕ Search

SEARCH · Engineering Papers

Results for “MONOCRYSTALS”

Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.

At least 1,783 records · Page 99

Surface texture of single-crystal silicon oxidized under a thin V{sub 2}O{sub 5} layer

The process of surface texturing of single-crystal silicon oxidized under a V{sub 2}O{sub 5} layer is studied. Intense silicon oxidation at the Si–V{sub 2}O{sub 5} interface begins at a temperature of 903 K which is 200 K below than upon silicon thermal oxidation in an oxygen atmosphere. A silicon dioxide layer 30–50 nm thick with SiO{sub 2} inclusions in silicon depth up to 400 nm is formed at the V{sub 2}O{sub 5}–Si interface. The diffusion coefficient of atomic oxygen through the silicon-dioxide layer at 903 K is determined (D ≥ 2 × 10{sup –15} cm{sup 2} s{sup –1}). A model of low-temperature silicon oxidation, based on atomic oxygen diffusion from V{sub 2}O{sub 5} through the SiO{sub 2} layer to silicon, and SiO{sub x} precipitate formation in silicon is proposed. After removing the V{sub 2}O{sub 5} and silicon-dioxide layers, texture is formed on the silicon surface, which intensely scatters light in the wavelength range of 300–550 nm and is important in the texturing of the front and rear surfaces of solar cells.

36 MATERIALS SCIENCE↗

Influence of the doping type and level on the morphology of porous Si formed by galvanic etching

The formation of porous silicon (por-Si) layers by the galvanic etching of single-crystal Si samples (doped with boron or phosphorus) in an HF/C{sub 2}H{sub 5}OH/H{sub 2}O{sub 2} solution is investigated. The por-Si layers are analyzed by the capillary condensation of nitrogen and scanning electron microscopy (SEM). The dependences of the morphological characteristics of por-Si (pore diameter, specific surface area, pore volume, and thickness of the pore walls), which determine the por-Si combustion kinetics, on the dopant type and initial wafer resistivity are established.

36 MATERIALS SCIENCE↗

Single crystals of (FeIn{sub 2}S{sub 4}){sub x} · (CuIn{sub 5}S{sub 8}){sub 1–x} alloys: Crystal structure, nuclear gamma resonance spectra, and thermal expansion

FeIn{sub 2}S{sub 4} and CuIn{sub 5}S{sub 8} compounds and (FeIn{sub 2}S{sub 4}){sub x} · (CuIn{sub 5}S{sub 8}){sub 1–x} alloy single crystals are grown by planar crystallization. It is shown that both of the initial FeIn{sub 2}S{sub 4} and CuIn{sub 5}S{sub 8} compounds and alloys on their basis crystallize with the formation of the cubic spinel structure. It is established that the unit-cell parameter a linearly varies with the composition parameter x. By means of nuclear gamma resonance spectroscopy in the transmission mode of measurements, the local states of iron ions in the alloys are studied. For the single crystals grown in the study, thermal expansion is explored using the dilatometry technique, the thermal-expansion coefficients are determined, and the Debye temperature and rms (root-mean-square) dynamic displacements are calculated.

36 MATERIALS SCIENCE↗

Crystal defects in solar cells produced by the method of thermomigration

The results of studying the crystal structure of regions in silicon, recrystallized during the course of thermomigration of the liquid Si–Al zone in the volume of the silicon substrate, are reported (similar regions doped with an acceptor impurity are used to obtain high-voltage solar cells). X-ray methods (including measurements of both diffraction-reflection curves and topograms) and also high-resolution electron microscopy indicate that single-crystal regions in the form of a series of thin strips or rectangular grids are formed as a result of the thermomigration of liquid zones. Dislocation half-loops are detected in the surface layers of the front and back surfaces of the substrate. (311)-type defects are observed in the recrystallized regions.

14 SOLAR ENERGY↗

Silicon nanowire array architecture for heterojunction electronics

Photosensitive nanostructured heterojunctions n-TiN/p-Si were fabricated by means of titanium nitride thin films deposition (n-type conductivity) by the DC reactive magnetron sputtering onto nano structured single crystal substrates of p-type Si (100). The temperature dependencies of the height of the potential barrier and series resistance of the n-TiN/p-Si heterojunctions were investigated. The dominant current transport mechanisms through the heterojunctions under investigation were determined at forward and reverse bias. The heterojunctions under investigation generate open-circuit voltage V{sub oc} = 0.8 V, short-circuit current I{sub sc} = 3.72 mA/cm{sup 2} and fill factor FF = 0.5 under illumination of 100 mW/cm{sup 2}.

36 MATERIALS SCIENCE↗

Effect of doping with rare-earth elements (Eu, Tb, Dy) on the conductivity of Bi{sub 2}Te{sub 3} layered single crystals

The temperature dependences of the resistivity in the directions parallel and perpendicular to the layer plane in the range of temperatures T = 5–300 K and the Hall and transverse magnetoresistance effects (magnetic fields <80 kOe, T = 5 K) are studied for doped and undoped Bi{sub 2}Te{sub 3} layered single crystals. It is shown that, upon the doping of Bi{sub 2}Te{sub 3} crystals with atoms of rare-earth elements (Eu, Tb, Dy), the resistivity in the directions parallel and perpendicular to the layer plane in Bi{sub 2}Te{sub 3} increases. The increase in the resistivity is caused mainly by a decrease in the charge-carrier mobility because of an increased contribution of charge-carrier scattering at defects to scattering processes. The charge-carrier concentrations and mobilities as well as the Hall factor defined by the anisotropy of the effective masses and by the orientation of ellipsoids with respect to the crystallographic axes are estimated.

36 MATERIALS SCIENCE↗

Structure of bismuth films obtained using an array of identically oriented single-crystal bismuth islands preliminarily grown on a substrate

An array of identically oriented single-crystal bismuth islands formed on mica plates is used as a substrate to improve the structure of bismuth thin films grown by vacuum thermal evaporation. The array of islands is formed by the chemical etching of a single-crystal bismuth film 1 μm thick grown by floating-zone recrystallization under a coating. The structure of the obtained films is studied by X-ray diffraction, atomicforce microscopy, and electron backscatter diffraction scanning electron microscopy.

36 MATERIALS SCIENCE↗

Mn{sub 0.1}Ag{sub 0.9}In{sub 4.7}S{sub 7.6} single crystals: Crystal structure, band gap, and thermal expansion

Mn{sub 0.1}Ag{sub 0.9}In{sub 4.7}S{sub 7.6} single crystals are for the first time grown by the Bridgman method (vertical variant). The single crystals crystallize in the cubic spinel structure. The band gap of the single crystals is determined from the transmittance spectra in the region of the fundamental absorption edge at temperatures of T = 295 and 80 K. Thermal expansion is studied by the dilatometric method in the temperature range 80–500 K. The coefficients of thermal expansion, the Debye temperatures, and the rms (root mean square) dynamic displacements of atoms are calculated.

36 MATERIALS SCIENCE↗

Optical thyristor based on GaAs/InGaP materials

The possibility of creating thyristor structures with external optical control by laser radiation with a wavelength of ~800 nm, based on single-crystal wafers of semi-insulating GaAs and layers of InGaP with the lattice parameter compatible with GaAs, is shown.

36 MATERIALS SCIENCE↗

Investigation of the Far-IR Reflection Spectra of SmS Single Crystals and Polycrystals in the Homogeneity Range

The far- and mid-IR reflection spectra of Sm{sub 1+} {sub x}S (x = 0–0.17) samples are recorded and analyzed, as well as their electrical and structural parameters at a temperature of T = 300 K. The bond ionicity in SmS is shown to fall with a decrease in the area of the X-ray coherent scattering region and an increase in the concentration of donor impurities and, consequently, conduction electron concentration. The electrical conductivity of stoichiometric SmS single crystals and polycrystals can be determined with an error of 10% from the IR reflection spectra. Due to the low structural quality of the samples, the electrical conductivity cannot be determined in the case of deviation from stoichiometry.

36 MATERIALS SCIENCE↗

On the Growth of FeIn{sub 2}S{sub 2}Se{sub 2} Single Crystals and the Study of their Properties

FeIn{sub 2}S{sub 2}Se{sub 2} single crystals are grown for the first time by the Bridgman method, and their composition and properties are determined. It is found that the single crystals are hexagonal in structure. The arrangement of Fe ions in the structure of the FeIn{sub 2}S{sub 2}Se{sub 2} crystals is studied by nuclear γ-resonance spectroscopy. From the transmittance spectra in the region of the fundamental absorption edge, the band gap of the single crystals grown in the study is determined.

36 MATERIALS SCIENCE↗

Features of the Electron Mobility in the n-InSe Layered Semiconductor

The dependences of the Hall electron mobility of n-InSe single crystals grown by the Bridgman method on a sample’s technological history, temperature, electric field, doping, and illumination are experimentally investigated. It is established that at temperatures below room temperature, the dependences of the electron mobility on external factors, initial resistivity, and doping are anomalous, i.e., do not obey the theory of free carrier mobility in quasi-ordered crystalline semiconductors. The observed anomalies are attributed to partial disordering and fluctuation of the potential of free energy bands of the n-InSe single crystals and can be controlled by temperature, electric field, doping, and illumination.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Effect of a por-Si Buffer Layer on the Structure and Morphology of Epitaxial In{sub x}Ga{sub 1 – x}N/Si(111) Heterostructures

Integrated heterostructures exhibiting nanocolumnar morphology of the In{sub x}Ga{sub 1 – x}N/Si(111) film are grown on a single-crystal silicon substrate (c-Si(111)) and a substrate with a nanoporous buffer sublayer (por-Si) by molecular-beam epitaxy with the plasma activation of nitrogen. Using a complex of structural and microscopic methods of analysis, it is shown that the growth of In{sub x}Ga{sub 1 – x}N nanocolumns on a nanoporous buffer layer offers a number of advantages over growth on c-Si. The por-Si substrate predetermines the preferential orientation of the growth of In{sub x}Ga{sub 1 – x}N nanocolumns closer to the Si(111) orientation direction and makes it possible to produce In{sub x}Ga{sub 1 – x}N nanocolumns with a higher degree of crystallographic uniformity and with a nanocolumn lateral size of ~40 nm unified over the entire surface. The growth of In{sub x}Ga{sub 1 – x}N nanocolumns on a por-Si layer yields a decrease in the strain components ε{sub xx} and ε{sub zz} and in the density of edge and screw dislocations compared to the corresponding parameters for In{sub x}Ga{sub 1 – x}N nanocolumns grown on c-Si. The In{sub x}Ga{sub 1 – x}N nanocolumnar layer fabricated on por-Si exhibits a 20% higher charge-carrier concentration compared to the layer grown on c-Si as well as a higher intensity of the photoluminescence quantum yield (+25%).

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

XAFS Investigation of Nanoparticle Formation in {sup 64}Zn{sup +} Ion Implanted and Thermo Oxidized Si

The single crystal CZ n-Si(100) substrates with electron concentration n{sub o} = 5 × 10{sup 16} cm{sup −3} were implanted by {sup 64}Zn{sup +} ions with dose of 5 × 10{sup 16} cm{sup −2} and energy of 50 keV. During implantation the ion beam current density was less than 0.5 μA/cm{sup 2} to avoid the substrate magnetically heating. After implantation, the plates were subjected to isochronous for one hour heat treatment in oxygen atmosphere at temperatures from 400 up to 1000{sup o}C with a step of 100{sup o}C. Zn K-edge EXAFS spectra were measured in fluorescent mode. Si(111) channel-cut monochromator was used for energy scanning; energy resolution ΔE/E = 2 × 10{sup –4}. According to Zn K-edge EXAFS data, all Zn implanted in Si at 900{sup o}C is fully oxidized: an absolute maximum of EXAFS Fourier transform at R ~ 1.6 Å corresponds to Zn–O distance. Based on XANES data, we suggest an interaction between implanted Zn atoms and Si support.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Heteroepitaxy of GaP Nucleation Layers on Si by Molecular Beam Epitaxy

The growth of single crystalline GaP nucleation and buffer layers on Si substrates by molecular-beam epitaxy is demonstrated. The use of two different regimes of migration-enhanced epitaxy was studied. It was found that p–n junctions can be created due to the interdiffusion during the growth of GaP layer on p-type Si substrate.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Study of the Effect of Doping with Iron on the Luminescence of Zinc-Selenide Single Crystals

The effect of doping with iron (thermal diffusion from a surface) on the luminescence of zinc-selenide single crystals in the wavelength range 0.44–0.72 μm and on the spatial distribution of luminescence centers are studied. By means of two-photon confocal microscopy, planar and volume maps of edge (exciton) and impurity–defect luminescence in the above-indicated spectral range are obtained for both doped and undoped crystals. It is shown that crystal regions containing a high iron concentration exhibit low-intensity luminescence in this range. It is found that, in the process of diffusion, several types of impurity–defect centers distributed in a complex way within the crystal bulk are formed. The nature of these centers is discussed.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗

Influence of a por-Si Buffer Layer on the Optical Properties of Epitaxial In{sub x}Ga{sub 1 –x}N/Si(111) Heterostructures with a Nanocolumnar Film Morphology

Integrated heterostructures exhibiting a nanocolumnar morphology of the In{sub x}Ga{sub 1 –x}N film are grown on a single-crystal silicon substrate (c-Si(111)) and a substrate with a nanoporous buffer sublayer (por-Si) by molecular-beam epitaxy with the plasma activation of nitrogen. Using a complex of spectroscopic methods of analysis, it is shown that the growth of In{sub x}Ga{sub 1 –x}N nanocolumns on the por-Si buffer layer offer a number of advantages over growth on the c-Si substrate. Raman and ultraviolet spectroscopy data support the inference about the growth of a nanocolumn structure and agree with the previously obtained X-ray diffraction (XRD) data indicative of the strained, unrelaxed state of the In{sub x}Ga{sub 1 –x}N layer. The growth of In{sub x}Ga{sub 1 –x}N nanocolumns on the por-Si layer positively influences the optical properties of the heterostructures. At the same half-width of the emission line in the photoluminescence spectrum, the emission intensity for the heterostructure sample grown on the por-Si buffer layer is ~25% higher than the emission intensity for the film grown on the c-Si substrate.

75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND↗