92 research outputs found
The Multisensor Array Based on Grown-On-Chip Zinc Oxide Nanorod Network for Selective Discrimination of Alcohol Vapors at Sub-ppm Range
We discuss the fabrication of gas-analytical multisensor arrays based on ZnO nanorods grown via a hydrothermal route directly on a multielectrode chip. The protocol to deposit the nanorods over the chip includes the primary formation of ZnO nano-clusters over the surface and secondly the oxide hydrothermal growth in a solution that facilitates the appearance of ZnO nanorods in the high aspect ratio which comprise a network. We have tested the proof-of-concept prototype of the ZnO nanorod network-based chip heated up to 400 Β°C versus three alcohol vapors, ethanol, isopropanol and butanol, at approx. 0.2β5 ppm concentrations when mixed with dry air. The results indicate that the developed chip is highly sensitive to these analytes with a detection limit down to the sub-ppm range. Due to the pristine differences in ZnO nanorod network density the chip yields a vector signal which enables the discrimination of various alcohols at a reasonable degree via processing by linear discriminant analysis even at a sub-ppm concentration range suitable for practical applications
Fractal analysis of the AFM-images of CuβGaβSe films, prepared by chemical bath deposition
Π‘ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π°ΡΠΎΠΌΠ½ΠΎ-ΡΠΈΠ»ΠΎΠ²ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π° ΠΌΠΎΡΡΠΎΠ»ΠΎΠ³ΠΈΡ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ CuβGaβSe, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΠΎΠ²ΠΌΠ΅ΡΡΠ½ΡΠΌ Π³ΠΈΠ΄ΡΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΠ΅ΠΌ ΡΠ΅Π»Π΅Π½ΠΈΠ΄ΠΎΠ² ΠΌΠ΅Π΄ΠΈ (I) Cu2Se ΠΈ Π³Π°Π»Π»ΠΈΡ Ga2Se3. Π‘ ΠΏΠΎΠΌΠΎΡΡΡ ΡΡΠ°ΠΊΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π½Π°Π»ΠΈΠ·Π° ΠΠ‘Π-ΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΠΉ ΡΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΡΡΠ»ΠΎΠ²ΠΈΡΠΌΠΈ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΡ ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ CuβGaβSe ΠΈ ΠΈΡ
ΡΡΠ°ΠΊΡΠ°Π»ΡΠ½ΠΎΠΉ ΡΠ°Π·ΠΌΠ΅ΡΠ½ΠΎΡΡΡΡ, ΡΠ°ΡΡΡΠΈΡΠ°Π½Π½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΠΏΠΎΠ΄ΡΡΠ΅ΡΠ° ΠΊΡΠ±ΠΎΠ² ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΡΠΈΠ°Π½Π³ΡΠ»ΡΡΠΈΠΈ. Π’Π°ΠΊΠΆΠ΅ ΠΏΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΡΠΎΡΡΠ° ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΏΡΠΈ Π³ΠΈΠ΄ΡΠΎΡ
ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΠΈ Π΄ΠΈΡΠ΅Π»Π΅Π½ΠΈΠ΄Π° ΠΌΠ΅Π΄ΠΈ (I) ΠΈ Π³Π°Π»Π»ΠΈΡ.The surface morphology of CuβGaβSe thin films prepared by chemical bath deposition of copper (I) Cu2Se and gallium selenides Ga2Se3 was investigated by means of an atomic-force microscopy. The dependence between the conditions of the deposition of CuβGaβSe thin films and their fractal dimension, calculated by counting cubes and by triangulation, was defined by means of fractal analysis. A mechanism for the formation and growth of films at chemical bath deposition of copper (I) and gallium selenides was proposed well as.ΠΡΠΎΠ³ΡΠ°ΠΌΠΌΠ° ΡΠ°Π·Π²ΠΈΡΠΈΡ Π£ΡΠ€Π£ Π½Π° 2013 Π³ΠΎΠ΄ (ΠΏ.1.2.2.3
ΠΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΡΠ΅Ρ ΠΌΠ΅ΡΠ½ΡΡ ΠΏΠΎΡΠΈΡΡΡΡ ΠΈΠ΅ΡΠ°ΡΡ ΠΈΡΠ΅ΡΠΊΠΈΡ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΡ ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ ΡΠ°ΠΌΠΎΡΠ±ΠΎΡΠΊΠΈ Π½Π°Π½ΠΎΡΡΠ΅Ρ
The article considers possibilities of using modeling fo r the development of two promising areas of modernΒ nanomaterials, i. e.Β materials with a hierarchy of pores organized hierarchical self- assembly and hierarchical structuresΒ with nanoporous elements. TheΒ pore size of hierarchical structures was estimated by means of quasi- two-dimensional projectionΒ of three-dimensional deterministic fractal Julien aggregate. Three-dimensional modeling of hierarchicalΒ structuresΒ organized by means of nanosphere self-assembly was conducted in the Autodesk 3ds Max environment. The article providesΒ analysis of dependences of porosity, density, specificΒ surface area of fractal structures on the size of aggregates (withΒ theΒ appearance of new pore levels of hierarchical materials),Β dependences of the porosity change in the case of replacementΒ of primary identical spherical particles on porous spheres.Π Π°ΡΡΠΌΠΎΡΡΠ΅Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π΄Π»Ρ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π΄Π²ΡΡ
ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠΉΒ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ Π½Π°Π½ΠΎΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ: ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² Ρ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΠ΅ΠΉ ΠΏΠΎΡ, ΡΠΎΠ±ΡΠ°Π½Π½ΡΡ
ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌΒ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ°ΠΌΠΎΡΠ±ΠΎΡΠΊΠΈ, Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΡΠΊΡΡΡ ΠΈΠ· Π½Π°Π½ΠΎΠΏΠΎΡΠΈΡΡΡΡ
Β ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ². Π‘ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌΒ ΠΊΠ²Π°Π·ΠΈΠ΄Π²ΡΠΌΠ΅ΡΠ½ΠΎΠΉ ΠΏΡΠΎΠ΅ΠΊΡΠΈΠΈ ΡΡΠ΅Ρ
ΠΌΠ΅ΡΠ½ΠΎΠ³ΠΎ Π΄Π΅ΡΠ΅ΡΠΌΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎΒ ΡΡΠ°ΠΊΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ Π°Π³ΡΠ΅Π³Π°ΡΠ° ΠΡΠ»ΡΠ΅Π½Π°Β ΠΎΡΠ΅Π½Π΅Π½ ΡΠ°Π·ΠΌΠ΅Ρ ΠΏΠΎΡ Π² ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΡΠΊΡΡΡΠ°Ρ
. Π’ΡΠ΅Ρ
ΠΌΠ΅ΡΠ½ΠΎΠ΅Β ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΡΡΡΠΊΡΡΡ, ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΡ
Β ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²ΠΎΠΌ ΡΠ°ΠΌΠΎΡΠ±ΠΎΡΠΊΠΈ Π½Π°Π½ΠΎΡΡΠ΅Ρ,Β ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π² ΡΡΠ΅Π΄Π΅ Autodesk 3ds Max. ΠΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½ΡΒ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΏΠΎΡΠΈΡΡΠΎΡΡΠΈ, ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ,Β ΡΠ΄Π΅Π»ΡΠ½ΠΎΠΉ ΠΏΠ»ΠΎΡΠ°Π΄ΠΈ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΡΡΠ°ΠΊΡΠ°Π»ΡΠ½ΡΡ
ΡΡΡΡΠΊΡΡΡ ΠΎΡ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠ²Β Π°Π³ΡΠ΅Π³Π°ΡΠΎΠ² (ΠΏΡΠΈΒ Π²ΠΎΠ·Π½ΠΈΠΊΠ½ΠΎΠ²Π΅Π½ΠΈΠΈ Π½ΠΎΠ²ΡΡ
ΡΡΠΎΠ²Π½Π΅ΠΉ ΠΏΠΎΡ ΠΈΠ΅ΡΠ°ΡΡ
ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ²), Π° ΡΠ°ΠΊΠΆΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡΒ ΠΏΠΎΡΠΈΡΡΠΎΡΡΠΈ ΠΏΡΠΈ Π·Π°ΠΌΠ΅Π½Π΅ ΠΏΠ΅ΡΠ²ΠΈΡΠ½ΡΡ
ΠΈΠ΄Π΅Π½ΡΠΈΡΠ½ΡΡ
ΡΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°ΡΡΠΈΡ Π½Π° ΠΏΠΎΡΠΈΡΡΡΠ΅ ΡΡΠ΅ΡΡ
Photoluminescence and its damping kinetics of nanoporous alumina m embranes formed in solutions of various carboxylic acids
The article is devoted to the study of the photoluminescence of carbon-containing anodic alumina obtained in various electrolytes based on carboxylic (tartaric and oxalic) acids. We studied the emission and excitation spectra of luminescence, as well as the PL decay of nanostructured anodic alumina membranes. It is shown that such membranes exhibit photoluminescence (excitation wavelength 330 nm) in the wavelength range 350-600 nm with a maximum at 460 nm. They have two PL centers with maxima at 440 and 490 nm and lifetimes of 0.2 and 4.0 ns, respectively. It is shown that the PL peak at 440 nm can be related to the emission of COOβ - ions, and the peak at 490 nm can be related to the PL of defects in partially oxidized amorphous carbon
The sorption of water molecules in the pores of anodic alumina films during aluminum anodizing in oxalic acid
The thermogravimetric analysis of membranes of anodic aluminum oxide (AAO) was carried out. The results showed that in the process of anodic growth, water molecules are adsorbed in the pores of Al2O3, the amount of which is determined by the anodizing voltage of aluminum. The relationship is revealed and the graphs of the relationship between anodizing voltage, annealing temperature, and weight loss of nanostructured membranes of AAO are presented. It has been established that the adsorption of water molecules on the surface of AAO is explained by the presence of a surface charge, which disappears after annealing at 200β300 Β°C. An increase in the amount of adsorbed water with an increase in the anodizing voltage from 20 to 40β
V indicates a decrease in the surface charge density
Results from the Indo-USSR ozonesonde intercomparison experiment
A total of seventeen vertical profiles of ozone were obtained during an Indo-USSR collaborative experiment on ozonesonde intercomparison conducted at Thumba during March 1983. The vertical distribution of ozone was measured using rocket-borne, balloon-borne as well as ground-based instruments. Four different rocket ozonesondes from India and USSR and the balloon ozonesonde were used to makein situ observations of ozone concentrations in addition to the Dobson spectrophotometric observations of total ozone and Umkehr. The rocket and the balloon launchings were effected in three salvos and measurements were made at different times of the day as well as during night. The results of all these measurements are used to obtain a mean ozone vertical distribution over Thumba foT the spring equinoxial period. The mean profile shows the maximum ozone concentration at 27 km with a value of (3.86Β±0-52)Γ1012 molecules per cc. Comparison of this mean profile with available satellite data for the equatorial regions shows that, in general, the Thumba values are lower by 10β15% at altitudes below 40 km and larger at altitudes above 50 km compared to the satellite results. The data also show evidence for a day-to-day variability and a possible day-to-night variability in the ozone vertical distribution with the night-time values higher than the daytime values at all altitudes above 35 km and the difference is found to increase with the increasing altitude
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅ΠΏΠ»ΠΎΠ²ΡΡ Ρ Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΈΠ· Π°Π»ΡΠΌΠΈΠ½ΠΈΡ Ρ Π½Π°Π½ΠΎΠΏΠΎΡΠΈΡΡΡΠΌ ΠΎΠΊΡΠΈΠ΄ΠΎΠΌ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ
In this work, we studied the thermal characteristics of flat heaters made of aluminum with a strip heating element in the form of carbon fiber. In order to provide the necessary insulation of the heating element from the metal base, a layer of porous anodic aluminum oxide with a thickness of 20 ΞΌm was formed on the aluminum surface. The ends of the carbon fiber filament were metallized with a layer of copper for subsequent soldering during the assembly of the electric heater. The carbon fiber filament of electric heater had an electrical resistance of 60 Ohms. Studies of the propagation of heat fluxes in the volume of a board made of aluminum with nanoporous aluminum oxide were carried out using thermal imaging measurements. The paper presents the dependence of temperature changes on the surface of the lid of a heating element made of aluminum and on the opposite side β heat transfer side with heating time. The results showed that the heat generated by a linear heating element of carbon fiber, quickly distributed throughout the entire volume of the aluminum plate of the heating element. This indicates a high thermal conductivity of the aluminum base of the heater, the parameters of which allow to achieve the required thermal characteristics of the heater.ΠΠ΄Π½ΠΎΠΉ ΠΈΠ· Π°ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π·Π°Π΄Π°Ρ Π² ΡΡΠ΅ΡΠ΅ ΡΡΠ°ΡΠΈΠΎΠ½Π°ΡΠ½ΠΎΠ³ΠΎ ΠΎΡΠΎΠΏΠ»Π΅Π½ΠΈΡ, Π½Π° ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΡΠΎΡΠΎΠΉ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Ρ ΡΡΠΈΠ»ΠΈΡ ΠΌΠ½ΠΎΠ³ΠΎΡΠΈΡΠ»Π΅Π½Π½ΡΡ
ΡΠ°Π·ΡΠ°Π±ΠΎΡΡΠΈΠΊΠΎΠ², ΡΠ²Π»ΡΠ΅ΡΡΡ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠΈ. ΠΠ°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΡΠ΅ ΡΠΈΡΡΠ΅ΠΌΡ ΠΌΠΎΠ³ΡΡ ΠΈΠΌΠ΅ΡΡ ΡΠ°ΠΌΡΠ΅ ΡΠ°Π·Π½ΠΎΠΎΠ±ΡΠ°Π·Π½ΡΠ΅ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΈ, Π½ΠΎ ΡΡΡΠ΅ΡΡΠ²ΡΡΡ ΠΎΡΠ½ΠΎΠ²Π½ΡΠ΅ ΡΡΠ΅Π±ΠΎΠ²Π°Π½ΠΈΡ ΠΊ ΠΈΡ
ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ΅, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ: ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΠ΅ Π²ΡΡΠΎΠΊΠΎΠΉ Π½Π°Π΄Π΅ΠΆΠ½ΠΎΡΡΠΈ ΠΏΡΠΈ ΡΠΊΡΠΏΠ»ΡΠ°ΡΠ°ΡΠΈΠΈ, ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ½ΠΎΡΡΡ, ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΡ ΠΊ Π²Π½Π΅ΡΠ½ΠΈΠΌ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡΠΌ ΠΈ ΡΡΠ°Π±ΠΈΠ»ΡΠ½ΠΎΡΡΡ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ. ΠΡΠ½ΠΎΠ²Π½ΠΎΠΉ ΡΠ»Π΅ΠΌΠ΅Π½Ρ Π»ΡΠ±ΠΎΠ³ΠΎ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΡΡΡΠΎΠΉΡΡΠ²Π° β Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»Ρ. Π Π½Π°ΡΡΠΎΡΡΠ΅Π΅ Π²ΡΠ΅ΠΌΡ ΠΏΠ»ΠΎΡΠΊΠΈΠ΅ ΡΠ΅Π·ΠΈΡΡΠΈΠ²Π½ΡΠ΅ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΠΈ Π½Π°ΡΠ»ΠΈ ΡΠΈΡΠΎΠΊΠΈΠΉ ΡΠΏΠ΅ΠΊΡΡ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ Π² Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΡΡ
ΡΡΡΡΠΎΠΉΡΡΠ²Π°Ρ
, ΠΏΡΠ΅Π΄Π½Π°Π·Π½Π°ΡΠ΅Π½Π½ΡΡ
Π΄Π»Ρ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π·Π΄ΠΎΡΠΎΠ²ΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΠΊΠ»ΠΈΠΌΠ°ΡΠ° Π² ΠΏΠΎΠΌΠ΅ΡΠ΅Π½ΠΈΡΡ
, ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠ°Π½ΠΈΡ Π·Π°Π΄Π°Π½Π½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² Π² ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠ΅ΡΡΠ°Ρ
, Π² ΡΠΈΡΡΠ΅ΠΌΠ°Ρ
Π°Π½ΡΠΈΠΎΠ±Π»Π΅Π΄Π΅Π½Π΅Π½ΠΈΡ, Π² ΡΠ΅Π»ΡΡΠΊΠΎΠΌ Ρ
ΠΎΠ·ΡΠΉΡΡΠ²Π΅ ΠΈ Π² ΠΏΡΠΎΠΌΡΡΠ»Π΅Π½Π½ΠΎΡΡΠΈ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ ΡΠ΅ΠΏΠ»ΠΎΠ²ΡΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΠΏΠ»ΠΎΡΠΊΠΈΡ
Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»Π΅ΠΉ, ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½Π½ΡΡ
ΠΈΠ· Π°Π»ΡΠΌΠΈΠ½ΠΈΡ, Ρ Π»Π΅Π½ΡΠΎΡΠ½ΡΠΌ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠΌ Π½Π°Π³ΡΠ΅Π²Π° Π² Π²ΠΈΠ΄Π΅ ΡΠ³Π»Π΅ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»ΠΎΠΊΠ½Π°. Π‘ ΡΠ΅Π»ΡΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΠΉ ΠΈΠ·ΠΎΠ»ΡΡΠΈΠΈ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΎΡ ΠΌΠ΅ΡΠ°Π»Π»ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΡ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π»ΠΈ ΡΠ»ΠΎΠΉ ΠΏΠΎΡΠΈΡΡΠΎΠ³ΠΎ Π°Π½ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΎΠΊΡΠΈΠ΄Π° Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΡΠΎΠ»ΡΠΈΠ½ΠΎΠΉ 20 ΠΌΠΊΠΌ. ΠΠΎΠ½ΡΡ Π½ΠΈΡΠΈ ΠΈΠ· ΡΠ³Π»Π΅ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»ΠΎΠΊΠ½Π° ΠΌΠ΅ΡΠ°Π»Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π»ΠΈ ΡΠ»ΠΎΠ΅ΠΌ ΠΌΠ΅Π΄ΠΈ Π΄Π»Ρ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΉ ΠΏΠ°ΠΉΠΊΠΈ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ ΡΠ±ΠΎΡΠΊΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»Ρ. ΠΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΠ΅ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»Ρ Ρ Π½ΠΈΡΡΡ ΠΈΠ· ΡΠ³Π»Π΅ΡΠΎΠ΄Π½ΠΎΠ³ΠΎ Π²ΠΎΠ»ΠΎΠΊΠ½Π° ΡΠΎΡΡΠ°Π²Π»ΡΠ»ΠΎ 60 ΠΠΌ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½ΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΠ²ΡΡ
ΠΏΠΎΡΠΎΠΊΠΎΠ² Π² ΠΎΠ±ΡΠ΅ΠΌΠ΅ ΠΏΠ»Π°ΡΡ ΠΈΠ· Π°Π»ΡΠΌΠΈΠ½ΠΈΡ Ρ Π½Π°Π½ΠΎΠΏΠΎΡΠΈΡΡΡΠΌ ΠΎΠΊΡΠΈΠ΄ΠΎΠΌ Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠ΅ΠΏΠ»ΠΎΠ²ΠΈΠ·ΠΈΠΎΠ½Π½ΡΡ
ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΠΉ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ Π½Π° ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΊΡΡΡΠΊΠΈ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΈΠ· Π°Π»ΡΠΌΠΈΠ½ΠΈΡ ΠΈ Π½Π° ΠΏΡΠΎΡΠΈΠ²ΠΎΠΏΠΎΠ»ΠΎΠΆΠ½ΠΎΠΉ ΡΠ΅ΠΏΠ»ΠΎΠΎΡΠ΄Π°ΡΡΠ΅ΠΉ ΡΡΠΎΡΠΎΠ½Π΅ ΠΎΡ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ Π½Π°Π³ΡΠ΅Π²Π°. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, ΡΡΠΎ ΡΠ΅ΠΏΠ»ΠΎ, Π³Π΅Π½Π΅ΡΠΈΡΡΠ΅ΠΌΠΎΠ΅ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΠΌ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΡΠΌ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠΌ ΠΈΠ· ΡΠ³Π»Π΅ΡΠΎΠ΄Π½ΠΎΠΉ Π½ΠΈΡΠΈ, Π±ΡΡΡΡΠΎ ΠΏΠ΅ΡΠ΅ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΡ ΠΏΠΎ Π²ΡΠ΅ΠΌΡ ΠΎΠ±ΡΠ΅ΠΌΡ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠΉ ΠΏΠ»Π°ΡΡΠΈΠ½Ρ Ρ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»ΡΠ½ΡΠΌ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠΌ. ΠΡΠΎ ΡΠ²ΠΈΠ΄Π΅ΡΠ΅Π»ΡΡΡΠ²ΡΠ΅Ρ ΠΎ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠ΅ΠΏΠ»ΠΎΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΎΡΡΠΈ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠΉ ΠΎΡΠ½ΠΎΠ²Ρ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»Ρ, ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΠΊΠΎΡΠΎΡΠΎΠΉ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΡΡ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΡΠ΅Π±ΡΠ΅ΠΌΡΡ
ΡΠ΅ΠΏΠ»ΠΎΠ²ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ Π½Π°Π³ΡΠ΅Π²Π°ΡΠ΅Π»Ρ
Influence of Electrolyte Temperature on the Formation of the Morphology of the Porous Structure of Anodic Aluminum Oxide
The results of research on anodizing thin aluminum films 100 nm thick on SiO2βSi plates at 30 V in a 0.3 M aqueous solution of oxalic acid are presented. The effect of the electrolyte temperature on the morphology of porous anodic aluminum oxide (PAAO) films is studied. The pore diameter and interpore distance are determined by the computer analysis of the SEM images of the morphology of the anode films using the ImageJ software. The data obtained show that the pore diameter does not depend on the temperature of the electrolyte and the time of the process, but is determined only by the anodizing voltage. In the electrolyte temperature range of 5 to 40Β°C, the pore diameter of the PAAO films is 20 Β± 0.5 nm, and the interpore distance is 77.7 nm. The research results indicate that a change in the temperature of the electrolyte, in contrast to the anodizing voltage, affects only the growth rate of the anode film, and not its porous morphology
- β¦