278 research outputs found
Quaternary palynostratigraphy of the Pechora Sea
By combining the lithologic, original palynologic and published micropaleonthological data we reconstructed paleogeographical events On the Pechora shelf during the Younger Dryas and Holocene time. Our paleoenvironmental reconstructions are based On the regularities in formation of pollen-and-spores assemblages in the surface sediments of the Pechora Sea. The main stages in paleogeography of the Pechora Sea during the Late Pleistocene were emphasized. The Late Valdai sediments in the Pechora Sea region were accumulated under the influence of fluvioglacial flows probably from the melting ice cap on Kolguev Island and, also, coastal glaciers. Climate deterioration considerably changed coastal vegetation as reflected in the depleted taxonomic and quantitative composition of palynospectra. The pollen data suggest that Open steppe-like plant communities with Artemisia, Poaceae, Asteraceae and Caryophyllaceae dominated dry ecotopes On watersheds, whereas tundra-like communities with Betula nana, arctic Salix, Dryas, Saxifraga, Carex and Brassicaceae were common in more humid coastal lowlands.
The overlying silts and loamy sands are believed to have been accumulated during early deglaciation, i.e., Older Dryas and AllerΓΆd. During this phase the glacial sedimentation was rather rapidly replaced by a glaciomarine deposition. Progressive climate warming caused prominent changes in coastal vegetation. Discontinuous treeless tundra-steppe associations were replaced by dwarf and shrub ernik tundra. A "complex vegetation cover" of forest-tundra apparently existed in the northern part of the Kola Peninsula and in the Northern Dvina Lowland. By the end of the AllerΓΆd alder-bushes and horsetails occupied riverbanks, and spruce occurred in the forest-tundra communities on the adjacent hinterland
Convergence modelling in international integration associations
The article considers mathematical tools for modelling economic policy as a whole, as well as convergence in the field of labor, foreign economic activity, monetary and debt policy. Convergence was estimated using the convergence model, which characterizes the decrease in time spread in the levels of development of countries and regions, reflecting the negative relationship between economic growth rates and the initial level of development of countries and regions. The convergence was estimated by the coefficient of variation and by the dispersion-based model. To assess convergence, we used the Barro and Salai- Martin models, as well as the Baumol, Solow-Svan, and Quadrado-Rour models. The use of this mathematical toolkit allows to explore the presence and speed of convergence before and after joining international integration associations. The proposed mathematical modelling tools are recommended to be used in order to analyze convergence processes, study the dynamics of convergence or divergence, and also to adjust the directions and methods of state and regional economic policies of countries included in the integration association. Β© 2020 South Ural State University. All rights reserved
Study of the surface profiling of silicon based on the method of local anodic oxidation using scanning probe microscopy
Π‘Π ΠΠΠΠΠΠΠ ΠΠΠ’Π ΠΠ§ΠΠ«Π₯ ΠΠ€Π€ΠΠΠ’ΠΠ ΠΠ ΠΠ’ΠΠΠΠ-ΠΠΠΠ‘Π‘ΠΠΠΠΠ«Π₯ Π‘ΠΠΠΠ’Π ΠΠΠΠ’Π ΠΠ₯ Π‘ ΠΠΠΠ ΠΠΠΠΠΠΠΠΠ ΠΠΠΠΠΠΠ
The creation and implementation of new sources of sample excitation and spectrometers based on them into the practice of analytical laboratories raises many questions for researchers about the obtained analytical characteristics of new equipment and analysis methods. The most important characteristics of any method include detection limits, accuracy and reproducibility of the results obtained. Matrix elements can have a significant effect on these parameters. The paper shows a comparison of the change in the intensities of analytical lines of elements in the presence of matrix elements with ionization potentials of 5.13 - 10.48 eV (Na, Cu, Pb, Cd, Zn, In, Ga, Bi) in the concentration range of 0 - 1 wt %. on commercially available atomic emission spectrometers with microwave plasma Grand-MP ("VMK-Optoelektronika") and Agilent MP-AES 4100 (Agilent Technologies). It is shown that the magnitude of the matrix effect in these excitation sources depends on the ionization potential of the matrix element and the total energy of the analyte line. A significant effect of matrix elements with a concentration of up to 1% wt. on the intensity of spectral lines of atoms and ions of the sample. Elements with medium and high ionization energies practically do not affect the intensity of atomic spectral lines of impurity elements and lead to a decrease in the intensity of ionic lines. The influence of easily ionized elements is more pronounced - both depressing and amplifying effects are observed, probably caused by both a change in the concentration of electrons in the plasma, leading to a linear change in the equilibrium between atoms and ions, and a decrease in the plasma temperature. An increase in the power supplied to the plasma on the Grand-MP spectrometer leads to a decrease in the effect of easily ionized elements on the intensity of the spectral lines of the elements. It is shown that the plasma in the Grand-MP spectrometer has better resistance to matrix influences as compared to the Agilent MP-AES 4100, which is associated with a large plasma volume and a higher input power.Keywords: atomic emission analysis, microwave plasma, spectrum excitation source, magnetron, resonator, spectrometer, analytical characteristics.Β DOI: http://dx.doi.org/10.15826/analitika.2021.25.4.004E.V. Polyakova1, O.V. Pelipasov21Nikolaev Institute of Inorganic Chemistry of the Siberian Branch of the Russian Academy of Sciences, 3, Lavrentiev ave., Novosibirsk, 630090, Russian Federation2Institute of Automation and Electrometry of the Siberian Branch of the Russian Academy of Sciences, 1, Academician Koptyug ave., Novosibirsk,Β 630090, Russian FederationΠ‘ΠΎΠ·Π΄Π°Π½ΠΈΠ΅ ΠΈ Π²Π½Π΅Π΄ΡΠ΅Π½ΠΈΠ΅ Π² ΠΏΡΠ°ΠΊΡΠΈΠΊΡ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠΈΠΈ Π½ΠΎΠ²ΡΡ
ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠ² Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΡ ΡΠΏΠ΅ΠΊΡΡΠΎΠ² ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π°ΡΠΎΠΌΠΎΠ² ΠΏΡΠΎΠ±Ρ ΠΈ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΎΠ² Π½Π° ΠΈΡ
ΠΎΡΠ½ΠΎΠ²Π΅ ΡΡΠ°Π²ΠΈΡ ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ²ΠΎ Π²ΠΎΠΏΡΠΎΡΠΎΠ² ΠΏΠ΅ΡΠ΅Π΄ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠΌΠΈ ΠΎ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°Ρ
Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΎΠ±ΠΎΡΡΠ΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊ Π°Π½Π°Π»ΠΈΠ·Π°. Π Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Π²Π°ΠΆΠ½ΡΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌ Π»ΡΠ±ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΎΡΠ½ΠΎΡΡΡ ΠΏΡΠ΅Π΄Π΅Π»Ρ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ, ΠΏΡΠ°Π²ΠΈΠ»ΡΠ½ΠΎΡΡΡ ΠΈ Π²ΠΎΡΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌΡΡ
ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ². Π‘ΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΡΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΠΌΠΎΠ³ΡΡ ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ ΠΌΠ°ΡΡΠΈΡΠ½ΡΠ΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΡ. Π ΡΠ°Π±ΠΎΡΠ΅ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠ΅ΠΉ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ²-ΠΏΡΠΈΠΌΠ΅ΡΠ΅ΠΉ Π² ΠΏΡΠΈΡΡΡΡΡΠ²ΠΈΠΈ ΠΌΠ°ΡΡΠΈΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Ρ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π°ΠΌΠΈ ΠΈΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ 5.13 β 10.48 ΡΠ (Na, Cu, Pb, Cd, Zn, In, Ga, Bi, P) Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΉ 0 β 1Β % ΠΌΠ°Ρ. Π½Π° ΠΊΠΎΠΌΠΌΠ΅ΡΡΠ΅ΡΠΊΠΈ Π΄ΠΎΡΡΡΠΏΠ½ΡΡ
Π°ΡΠΎΠΌΠ½ΠΎ-ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½ΡΡ
ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠ°Ρ
Ρ ΠΌΠΈΠΊΡΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ ΠΏΠ»Π°Π·ΠΌΠΎΠΉ Β«ΠΡΠ°Π½Π΄-Π‘ΠΠ§Β» (Β«ΠΠΠ-ΠΠΏΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠ°Β») ΠΈ Agilent MP-AES 4100 (Agilent Technologies). ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π²Π΅Π»ΠΈΡΠΈΠ½Π° ΠΌΠ°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΡΡΡΠ΅ΠΊΡΠ° Π² ΡΡΠΈΡ
ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ°Ρ
Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΡ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π° ΠΈΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠ°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΈ ΡΡΠΌΠΌΠ°ΡΠ½ΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π»ΠΈΠ½ΠΈΠΈ Π°Π½Π°Π»ΠΈΡΠ°. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΌΠ°ΡΡΠΈΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² (Na, Cu, Pb, Cd, Zn, In, Ga, Bi, P) Ρ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠ΅ΠΉ Π΄ΠΎ 1 % ΠΌΠ°Ρ. Π½Π° ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ Π°ΡΠΎΠΌΠΎΠ² ΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΏΡΠΎΠ±Ρ. ΠΠ»Π΅ΠΌΠ΅Π½ΡΡ ΡΠΎ ΡΡΠ΅Π΄Π½Π΅ΠΉ ΠΈ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠ΅ΠΉ ΠΈΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ Π²Π»ΠΈΡΡΡ Π½Π° ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ Π°ΡΠΎΠΌΠ°ΡΠ½ΡΡ
ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ²-ΠΏΡΠΈΠΌΠ΅ΡΠ΅ΠΉ ΠΈ ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½Π½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ. ΠΠ»ΠΈΡΠ½ΠΈΠ΅ Π»Π΅Π³ΠΊΠΎΠΈΠΎΠ½ΠΈΠ·ΠΈΡΡΠ΅ΠΌΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΎ: Π½Π°Π±Π»ΡΠ΄Π°ΡΡΡΡ ΠΊΠ°ΠΊ Π΄Π΅ΠΏΡΠ΅ΡΡΠΈΡΡΡΡΠ΅Π΅, ΡΠ°ΠΊ ΠΈ ΡΡΠΈΠ»ΠΈΠ²Π°ΡΡΠ΅Π΅ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅, Π²ΡΠ·Π²Π°Π½Π½ΡΠ΅, Π²Π΅ΡΠΎΡΡΠ½ΠΎ, ΠΊΠ°ΠΊ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Π² ΠΏΠ»Π°Π·ΠΌΠ΅, ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡΠΈΠΌ ΠΊ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°Π²Π½ΠΎΠ²Π΅ΡΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ Π°ΡΠΎΠΌΠ°ΠΌΠΈ ΠΈ ΠΈΠΎΠ½Π°ΠΌΠΈ, ΡΠ°ΠΊ ΠΈ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΏΠ»Π°Π·ΠΌΡ. Π£Π²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ΄Π²ΠΎΠ΄ΠΈΠΌΠΎΠΉ ΠΊ ΠΏΠ»Π°Π·ΠΌΠ΅ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ Π½Π° ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠ΅ Β«ΠΡΠ°Π½Π΄-Π‘ΠΠ§Β» ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ Π²Π»ΠΈΡΠ½ΠΈΡ Π»Π΅Π³ΠΊΠΎΠΈΠΎΠ½ΠΈΠ·ΠΈΡΡΠ΅ΠΌΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Π½Π° ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ². ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΠ»Π°Π·ΠΌΠ° Π² ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠ΅ Β«ΠΡΠ°Π½Π΄-Π‘ΠΠ§Β» ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ Π»ΡΡΡΠ΅ΠΉ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΡΡ ΠΊ ΠΌΠ°ΡΡΠΈΡΠ½ΡΠΌ Π²Π»ΠΈΡΠ½ΠΈΡΠΌ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Agilent MP-AES 4100, ΡΡΠΎ ΡΠ²ΡΠ·Π°Π½ΠΎ Ρ Π±ΠΎΠ»ΡΡΠΈΠΌ ΠΎΠ±ΡΠ΅ΠΌΠΎΠΌ ΠΏΠ»Π°Π·ΠΌΡ ΠΈ Π±ΠΎΠ»ΡΡΠ΅ΠΉ ΠΏΠΎΠ΄Π²ΠΎΠ΄ΠΈΠΌΠΎΠΉ ΠΌΠΎΡΠ½ΠΎΡΡΡΡ.ΠΠ»ΡΡΠ΅Π²ΡΠ΅ ΡΠ»ΠΎΠ²Π°. ΠΡΠΎΠΌΠ½ΠΎ-ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½Π°Ρ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΈΡ, ΠΌΠΈΠΊΡΠΎΠ²ΠΎΠ»Π½ΠΎΠ²Π°Ρ ΠΏΠ»Π°Π·ΠΌΠ°, ΠΌΠ°Π³Π½Π΅ΡΡΠΎΠ½, ΠΌΠ°ΡΡΠΈΡΠ½ΡΠ΅ ΡΡΡΠ΅ΠΊΡΡ, Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠ°Ρ Ρ
ΠΈΠΌΠΈΡDOI: http://dx.doi.org/10.15826/analitika.2021.25.4.00
Masking layer formation on silicon substrate by the focused ion beams method for plasma-chemical treatment
Comparison of matrix effects on atomic emission spectrometers with nitrogen microwave induced plasma
Π‘ΠΎΠ·Π΄Π°Π½ΠΈΠ΅ ΠΈ Π²Π½Π΅Π΄ΡΠ΅Π½ΠΈΠ΅ Π² ΠΏΡΠ°ΠΊΡΠΈΠΊΡ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π»Π°Π±ΠΎΡΠ°ΡΠΎΡΠΈΠΈ Π½ΠΎΠ²ΡΡ
ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠ² Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΡ ΡΠΏΠ΅ΠΊΡΡΠΎΠ² ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π°ΡΠΎΠΌΠΎΠ² ΠΏΡΠΎΠ±Ρ ΠΈ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠΎΠ² Π½Π° ΠΈΡ
ΠΎΡΠ½ΠΎΠ²Π΅ ΡΡΠ°Π²ΠΈΡ ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ²ΠΎ Π²ΠΎΠΏΡΠΎΡΠΎΠ² ΠΏΠ΅ΡΠ΅Π΄ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠΌΠΈ ΠΎ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°Ρ
Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΎΠ±ΠΎΡΡΠ΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊ Π°Π½Π°Π»ΠΈΠ·Π°. Π Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Π²Π°ΠΆΠ½ΡΠΌ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌ Π»ΡΠ±ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° ΠΎΡΠ½ΠΎΡΡΡ ΠΏΡΠ΅Π΄Π΅Π»Ρ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ, ΠΏΡΠ°Π²ΠΈΠ»ΡΠ½ΠΎΡΡΡ ΠΈ Π²ΠΎΡΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠΌΠΎΡΡΡ ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌΡΡ
ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ². Π‘ΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΡΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΠΌΠΎΠ³ΡΡ ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ ΠΌΠ°ΡΡΠΈΡΠ½ΡΠ΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΡ. Π ΡΠ°Π±ΠΎΡΠ΅ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠ΅ΠΉ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ²-ΠΏΡΠΈΠΌΠ΅ΡΠ΅ΠΉ Π² ΠΏΡΠΈΡΡΡΡΡΠ²ΠΈΠΈ ΠΌΠ°ΡΡΠΈΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Ρ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π°ΠΌΠΈ ΠΈΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ 5.13 - 10.48 ΡΠ (Na, Cu, Pb, Cd, Zn, In, Ga, Bi, P) Π² Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΉ 0 - 1 % ΠΌΠ°Ρ. Π½Π° ΠΊΠΎΠΌΠΌΠ΅ΡΡΠ΅ΡΠΊΠΈ Π΄ΠΎΡΡΡΠΏΠ½ΡΡ
Π°ΡΠΎΠΌΠ½ΠΎ-ΡΠΌΠΈΡΡΠΈΠΎΠ½Π½ΡΡ
ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠ°Ρ
Ρ ΠΌΠΈΠΊΡΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ ΠΏΠ»Π°Π·ΠΌΠΎΠΉ Β«ΠΡΠ°Π½Π΄-Π‘ΠΠ§Β» (Β«ΠΠΠ-ΠΠΏΡΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠ°Β») ΠΈ Agilent MP-AES 4100 (Agilent Technologies). ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ Π²Π΅Π»ΠΈΡΠΈΠ½Π° ΠΌΠ°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΡΡΡΠ΅ΠΊΡΠ° Π² ΡΡΠΈΡ
ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ°Ρ
Π²ΠΎΠ·Π±ΡΠΆΠ΄Π΅Π½ΠΈΡ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ ΠΏΠΎΡΠ΅Π½ΡΠΈΠ°Π»Π° ΠΈΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ ΠΌΠ°ΡΡΠΈΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ° ΠΈ ΡΡΠΌΠΌΠ°ΡΠ½ΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠΈ Π»ΠΈΠ½ΠΈΠΈ Π°Π½Π°Π»ΠΈΡΠ°. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΌΠ°ΡΡΠΈΡΠ½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² (Na, Cu, Pb, Cd, Zn, In, Ga, Bi, P) Ρ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠ΅ΠΉ Π΄ΠΎ 1 % ΠΌΠ°Ρ. Π½Π° ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ Π°ΡΠΎΠΌΠΎΠ² ΠΈ ΠΈΠΎΠ½ΠΎΠ² ΠΏΡΠΎΠ±Ρ. ΠΠ»Π΅ΠΌΠ΅Π½ΡΡ ΡΠΎ ΡΡΠ΅Π΄Π½Π΅ΠΉ ΠΈ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠ½Π΅ΡΠ³ΠΈΠ΅ΠΉ ΠΈΠΎΠ½ΠΈΠ·Π°ΡΠΈΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΈ Π½Π΅ Π²Π»ΠΈΡΡΡ Π½Π° ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ Π°ΡΠΎΠΌΠ°ΡΠ½ΡΡ
ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ²-ΠΏΡΠΈΠΌΠ΅ΡΠ΅ΠΉ ΠΈ ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΈΠΎΠ½Π½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ. ΠΠ»ΠΈΡΠ½ΠΈΠ΅ Π»Π΅Π³ΠΊΠΎΠΈΠΎΠ½ΠΈΠ·ΠΈΡΡΠ΅ΠΌΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΎ: Π½Π°Π±Π»ΡΠ΄Π°ΡΡΡΡ ΠΊΠ°ΠΊ Π΄Π΅ΠΏΡΠ΅ΡΡΠΈΡΡΡΡΠ΅Π΅, ΡΠ°ΠΊ ΠΈ ΡΡΠΈΠ»ΠΈΠ²Π°ΡΡΠ΅Π΅ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅, Π²ΡΠ·Π²Π°Π½Π½ΡΠ΅, Π²Π΅ΡΠΎΡΡΠ½ΠΎ, ΠΊΠ°ΠΊ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΎΠ² Π² ΠΏΠ»Π°Π·ΠΌΠ΅, ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡΠΈΠΌ ΠΊ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌΡ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°Π²Π½ΠΎΠ²Π΅ΡΠΈΡ ΠΌΠ΅ΠΆΠ΄Ρ Π°ΡΠΎΠΌΠ°ΠΌΠΈ ΠΈ ΠΈΠΎΠ½Π°ΠΌΠΈ, ΡΠ°ΠΊ ΠΈ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΡ ΠΏΠ»Π°Π·ΠΌΡ. Π£Π²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΠΏΠΎΠ΄Π²ΠΎΠ΄ΠΈΠΌΠΎΠΉ ΠΊ ΠΏΠ»Π°Π·ΠΌΠ΅ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ Π½Π° ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠ΅ Β«ΠΡΠ°Π½Π΄-Π‘ΠΠ§Β» ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ Π²Π»ΠΈΡΠ½ΠΈΡ Π»Π΅Π³ΠΊΠΎΠΈΠΎΠ½ΠΈΠ·ΠΈΡΡΠ΅ΠΌΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Π½Π° ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ². ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΏΠ»Π°Π·ΠΌΠ° Π² ΡΠΏΠ΅ΠΊΡΡΠΎΠΌΠ΅ΡΡΠ΅ Β«ΠΡΠ°Π½Π΄-Π‘ΠΠ§Β» ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ Π»ΡΡΡΠ΅ΠΉ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΡΡ ΠΊ ΠΌΠ°ΡΡΠΈΡΠ½ΡΠΌ Π²Π»ΠΈΡΠ½ΠΈΡΠΌ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Agilent MP-AES 4100, ΡΡΠΎ ΡΠ²ΡΠ·Π°Π½ΠΎ Ρ Π±ΠΎΠ»ΡΡΠΈΠΌ ΠΎΠ±ΡΠ΅ΠΌΠΎΠΌ ΠΏΠ»Π°Π·ΠΌΡ ΠΈ Π±ΠΎΠ»ΡΡΠ΅ΠΉ ΠΏΠΎΠ΄Π²ΠΎΠ΄ΠΈΠΌΠΎΠΉ ΠΌΠΎΡΠ½ΠΎΡΡΡΡ.The creation and implementation of new sources of sample excitation and spectrometers based on them into the practice of analytical laboratories raises many questions for researchers about the obtained analytical characteristics of new equipment and analysis methods. The most important characteristics of any method include detection limits, accuracy and reproducibility of the results obtained. Matrix elements can have a significant effect on these parameters. The paper shows a comparison of the change in the intensities of analytical lines of elements in the presence of matrix elements with ionization potentials of 5.13 - 10.48 eV (Na, Cu, Pb, Cd, Zn, In, Ga, Bi) in the concentration range of 0 - 1 wt %. on commercially available atomic emission spectrometers with microwave plasma Grand-MP ("VMK-Optoelektronika") and Agilent MP-AES 4100 (Agilent Technologies). It is shown that the magnitude of the matrix effect in these excitation sources depends on the ionization potential of the matrix element and the total energy of the analyte line. A significant effect of matrix elements with a concentration of up to 1% wt. on the intensity of spectral lines of atoms and ions of the sample. Elements with medium and high ionization energies practically do not affect the intensity of atomic spectral lines of impurity elements and lead to a decrease in the intensity of ionic lines. The influence of easily ionized elements is more pronounced - both depressing and amplifying effects are observed, probably caused by both a change in the concentration of electrons in the plasma, leading to a linear change in the equilibrium between atoms and ions, and a decrease in the plasma temperature. An increase in the power supplied to the plasma on the Grand-MP spectrometer leads to a decrease in the effect of easily ionized elements on the intensity of the spectral lines of the elements. It is shown that the plasma in the Grand-MP spectrometer has better resistance to matrix influences as compared to the Agilent MP-AES 4100, which is associated with a large plasma volume and a higher input power
Economic and mathematical modeling of regional industrial processes
The paper presents a method for the parallel optimization of the structure of sown areas for calculating economic and mathematical models for the traditional and organic-oriented land use systems characterized by the introduction of an additional set of environmental criteria constraints.
Based on the proposed methodology, an economic-mathematical model has been calculated and the effectiveness of the functioning of the Altai Foothills zonal agroecocluster has been proved.
Considering the full involvement in the agricultural production turnover of land suitable to produce organic products, the level of profitability was 39.7% against 17.3% in case of optimizing the structure of the sown areas in the traditional system of agricultural production.peer-reviewe
Singularities, Lax degeneracies and Maslov indices of the periodic Toda chain
The n-particle periodic Toda chain is a well known example of an integrable
but nonseparable Hamiltonian system in R^{2n}. We show that Sigma_k, the k-fold
singularities of the Toda chain, ie points where there exist k independent
linear relations amongst the gradients of the integrals of motion, coincide
with points where there are k (doubly) degenerate eigenvalues of
representatives L and Lbar of the two inequivalent classes of Lax matrices
(corresponding to degenerate periodic or antiperiodic solutions of the
associated second-order difference equation). The singularities are shown to be
nondegenerate, so that Sigma_k is a codimension-2k symplectic submanifold.
Sigma_k is shown to be of elliptic type, and the frequencies of transverse
oscillations under Hamiltonians which fix Sigma_k are computed in terms of
spectral data of the Lax matrices. If mu(C) is the (even) Maslov index of a
closed curve C in the regular component of R^{2n}, then (-1)^{\mu(C)/2} is
given by the product of the holonomies (equal to +/- 1) of the even- (or odd-)
indexed eigenvector bundles of L and Lmat.Comment: 25 pages; published versio
TEACHER TRAINING IN THE DEVELOPMENT OF INCLUSIVE EDUCATION IN MEDICAL SCHOOLS
The article highlights the experience of implementing inclusive education practices in higher medical schools: issues and methodological organization of psychological and pedagogical support of students with disabilities and disability faced by teachers embarking on their learning process.Π ΡΡΠ°ΡΡΠ΅ ΠΎΡΠ²Π΅ΡΠ°Π΅ΡΡΡ ΠΎΠΏΡΡ Π²Π½Π΅Π΄ΡΠ΅Π½ΠΈΡ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΠ½ΠΊΠ»ΡΠ·ΠΈΠ²Π½ΠΎΠ³ΠΎ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ Π² ΠΏΡΠ°ΠΊΡΠΈΠΊΡ Π²ΡΡΡΠ΅ΠΉ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠΉ ΡΠΊΠΎΠ»Ρ: Π²ΠΎΠΏΡΠΎΡΠ°ΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·Π°ΡΠΈΠΈ ΠΈ ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΎ-ΠΏΠ΅Π΄Π°Π³ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π΅Π½ΠΈΡ ΡΡΡΠ΄Π΅Π½ΡΠΎΠ² Ρ ΠΠΠ ΠΈ ΠΈΠ½Π²Π°Π»ΠΈΠ΄Π½ΠΎΡΡΡΡ, Ρ ΠΊΠΎΡΠΎΡΡΠΌΠΈ ΡΡΠ°Π»ΠΊΠΈΠ²Π°ΡΡΡΡ ΠΏΡΠ΅ΠΏΠΎΠ΄Π°Π²Π°ΡΠ΅Π»ΠΈ, ΠΏΡΠΈΡΡΡΠΏΠ°ΡΡΠΈΠ΅ ΠΊ ΠΏΡΠΎΡΠ΅ΡΡΡ ΠΈΡ
ΠΎΠ±ΡΡΠ΅Π½ΠΈΡ
- β¦