26 research outputs found
Π’Π΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΡΠΉ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½Ρ ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ ΡΠ΅Π΄ΠΊΠΎΠ·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΠΌΠΈ Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ
The regularities of changes in the concentration of an electrically active dopant in a nanostructured silicon film by changing the electrical resistivity depending on the doping conditions were investigated. The dependences of the changes in the obtained structures doped with rare-earth elements, such as La, Eu, Sm, Dy, Gd (lanthanides), on nanostructured silicon films are determined. The regularities of the obtained films changes and the temperature coefficient of resistance (TCR) change depending on the formation conditions are established. The regularities of the TCR are shown depending on the selected conditions for doping or non-doping of nanostructured silicon films with various impurities. It is shown that the main conditions under which the effect and change in the temperature coefficient of resistors resistance on thin films using rare-earth elements, such as oxygen, boron and phosphorus in the bulk of the film, is considered to be the temperature effect after deposition.ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈΡΡ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΠΎΠΉ Π»Π΅Π³ΠΈΡΡΡΡΠ΅ΠΉ ΠΏΡΠΈΠΌΠ΅ΡΠΈ Π² ΠΏΠ»Π΅Π½ΠΊΠ΅ Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, ΠΏΡΡΠ΅ΠΌ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΄Π΅Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΡΡΡΠΊΡΡΡ, Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΠ΅Π΄ΠΊΠΎΠ·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΠΌΠΈ (Π ΠΠ), ΡΠ°ΠΊΠΈΠΌΠΈ ΠΊΠ°ΠΊ La, Eu, Sm, Dy, Gd (Π»Π°Π½ΡΠ°Π½ΠΎΠΈΠ΄Ρ), Π½Π° Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠ»Π΅Π½ΠΊΠ°Ρ
ΠΊΡΠ΅ΠΌΠ½ΠΈΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ (Π’ΠΠ‘) Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ Π’ΠΠ‘ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π²ΡΠ±ΡΠ°Π½Π½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ»ΠΈ Π½Π΅Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΠΏΡΠΈΠΌΠ΅ΡΡΠΌΠΈ Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΎΡΠ½ΠΎΠ²Π½ΡΠΌΠΈ ΡΡΠ»ΠΎΠ²ΠΈΡΠΌΠΈ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΡΡ
ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ ΡΠ΅Π·ΠΈΡΡΠΎΡΠΎΠ² Π½Π° ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΊΠ°Ρ
Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π ΠΠ, ΡΠ°ΠΊΠΈΡ
ΠΊΠ°ΠΊ ΠΊΠΈΡΠ»ΠΎΡΠΎΠ΄, Π±ΠΎΡ ΠΈ ΡΠΎΡΡΠΎΡ, Π² ΠΎΠ±ΡΠ΅ΠΌΠ΅ ΠΏΠ»Π΅Π½ΠΊΠΈ, ΡΡΠΈΡΠ°Π΅ΡΡΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠΆΠ΅ ΠΏΠΎΡΠ»Π΅ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΡ
Temperature resistance coefficient of doped with rare earth elements nanostructured silicon films
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈΡΡ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΠΎΠΉ
Π»Π΅Π³ΠΈΡΡΡΡΠ΅ΠΉ ΠΏΡΠΈΠΌΠ΅ΡΠΈ Π² ΠΏΠ»Π΅Π½ΠΊΠ΅ Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ, ΠΏΡΡΠ΅ΠΌ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ΄Π΅Π»ΡΠ½ΠΎΠ³ΠΎ
ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΡΡΡΡΠΊΡΡΡ, Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΠ΅Π΄ΠΊΠΎΠ·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΠΌΠΈ (Π ΠΠ), ΡΠ°ΠΊΠΈΠΌΠΈ ΠΊΠ°ΠΊ
La, Eu, Sm, Dy, Gd (Π»Π°Π½ΡΠ°Π½ΠΎΠΈΠ΄Ρ), Π½Π° Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠ»Π΅Π½ΠΊΠ°Ρ
ΠΊΡΠ΅ΠΌΠ½ΠΈΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ
Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ°
ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ (Π’ΠΠ‘) Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½Ρ Π·Π°ΠΊΠΎΠ½ΠΎΠΌΠ΅ΡΠ½ΠΎΡΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ
Π’ΠΠ‘ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ Π²ΡΠ±ΡΠ°Π½Π½ΡΡ
ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ»ΠΈ Π½Π΅Π»Π΅Π³ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΠΏΡΠΈΠΌΠ΅ΡΡΠΌΠΈ
Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΏΠ»Π΅Π½ΠΎΠΊ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΠΎΡΠ½ΠΎΠ²Π½ΡΠΌΠΈ ΡΡΠ»ΠΎΠ²ΠΈΡΠΌΠΈ, ΠΏΡΠΈ ΠΊΠΎΡΠΎΡΡΡ
ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ
Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½ΡΠ° ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ ΡΠ΅Π·ΠΈΡΡΠΎΡΠΎΠ² Π½Π° ΡΠΎΠ½ΠΊΠΈΡ
ΠΏΠ»Π΅Π½ΠΊΠ°Ρ
Ρ
ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π ΠΠ, ΡΠ°ΠΊΠΈΡ
ΠΊΠ°ΠΊ ΠΊΠΈΡΠ»ΠΎΡΠΎΠ΄, Π±ΠΎΡ ΠΈ ΡΠΎΡΡΠΎΡ, Π² ΠΎΠ±ΡΠ΅ΠΌΠ΅ ΠΏΠ»Π΅Π½ΠΊΠΈ, ΡΡΠΈΡΠ°Π΅ΡΡΡ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ΅
Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠΆΠ΅ ΠΏΠΎΡΠ»Π΅ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΡ.The regularities of changes in the concentration of an electrically active dopant in a nanostructured
silicon film by changing the electrical resistivity depending on the doping conditions were investigated. The
dependences of the changes in the obtained structures doped with rare-earth elements, such as
La, Eu, Sm, Dy, Gd (lanthanides), on nanostructured silicon films are determined. The regularities of the
obtained films changes and the temperature coefficient of resistance (TCR) change depending on the formation
conditions are established. The regularities of the TCR are shown depending on the selected conditions for
doping or non-doping of nanostructured silicon films with various impurities. It is shown that the main
conditions under which the effect and change in the temperature coefficient of resistors resistance on thin films
using rare-earth elements, such as oxygen, boron and phosphorus in the bulk of the film, is considered to be the
temperature effect after deposition
ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΠΠ’-ΡΠ΅Ρ Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ Π΄Π»Ρ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΡΡ ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌ Π² ΡΠΎΡΠΌΠ΅ ΡΠΎΠΈΡΠΊΠ°ΡΠ΅Π»ΡΡΡΠ²Π° ΠΈ Π² ΡΠ°ΠΌΠΊΠ°Ρ Π°ΡΠΏΠΈΡΠ°Π½ΡΡΡΡ Π΄Π»Ρ ΠΈΠ½ΠΎΡΡΡΠ°Π½Π½ΡΡ Π³ΡΠ°ΠΆΠ΄Π°Π½
Factors affecting the effectiveness of video surveillance systems are considered, surveillance zones and blind zones calculating algorithms and their use in the developed program are presented
Π ΠΠΠΠΠΠΠΠΠ ΠΠΠΠΠΠΠΠ ΠΠΠΠ ΠΠ ΠΠΠΠΠ― Π ΠΠΠ ΠΠΠΠΠ― Π‘ ΠΠ‘ΠΠΠΠ¬ΠΠΠΠΠΠΠΠ ΠΠΠΠ’ΠΠΠ-Π ΠΠΠΠΠΠΠ Π¨ΠΠΠΠΠΠ Π ΠΠΠ§ΠΠ‘Π’ΠΠ ΠΠΠ’ΠΠΠΠΠΠ’ΠΠ Π
High degree of intensification of monohydrides decomposition process with use of catalysts is shown. It is established that the completeness decomposition of monohydrides in the presenceof platinoreniyevy spinel increases for 35-55 %.ΠΠΎΠΊΠ°Π·Π°Π½Π° Π²ΡΡΠΎΠΊΠ°Ρ ΡΡΠ΅ΠΏΠ΅Π½Ρ ΠΈΠ½ΡΠ΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΡ ΠΌΠΎΠ½ΠΎΠ³ΠΈΠ΄ΡΠΈΠ΄ΠΎΠ² Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΊΠ°ΡΠ°Π»ΠΈΠ·Π°ΡΠΎΡΠΎΠ². Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΠΏΠΎΠ»Π½ΠΎΡΠ° ΠΏΡΠΈ ΡΠ°Π·Π»ΠΎΠΆΠ΅Π½ΠΈΠΈ ΠΌΠΎΠ½ΠΎΠ³ΠΈΠ΄ΡΠΈΠ΄ΠΎΠ² Π² ΠΏΡΠΈΡΡΡΡΡΠ²ΠΈΠΈ ΠΏΠ»Π°ΡΠΈΠ½ΠΎΡΠ΅Π½ΠΈΠ΅Π²ΠΎΠΉ ΡΠΏΠΈΠ½Π΅Π»ΠΈ Π²ΠΎΠ·ΡΠ°ΡΡΠ°Π΅Ρ Π½Π° 35-55%
ΠΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½Π°Ρ ΠΎΡΠ΅Π½ΠΊΠ° ΡΠ΅ΡΠ΅Π²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π΄Π΅ΡΠ΅ΠΉ, Π·Π°ΡΠ°ΡΡΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΊΡΡΡΠ°ΠΊΠΎΡΠΏΠΎΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΠΏΠ»ΠΎΠ΄ΠΎΡΠ²ΠΎΡΠ΅Π½ΠΈΡ
Introduction. The high frequency of the use of assisted reproductive technologies and the inconsistency of information about the parameters of the cognitive development of IVF children determined the formulation of the research problem.The purpose of the work is to assess the originality of the speech development of children and adolescents conceived using the IVF procedure. The age of the children at the time of the survey was from 5 to 15 years.Methods and materials. A sample of 51 children (29 boys), mean age (7.9Β±2.8) years, 14 children had psychiatric diagnoses (ASD, mental retardation, etc.). Research methods: speech therapy assessment of speech development, neuropsychological diagnostics according to L.S. Tsvetkova, WICS, descriptive statistics, correlation analysis.Results. 41% of children had mild variants of speech development delay under 3 years old, 59 % of children had normal speech development. With age, the frequency of detected deviations in speech development decreases, so that in older age group (from 11 to 15 years old), 85 % have normotypical development of speech. Correlation analysis showed the originality of the correlations of the parameters of speech development, neuropsychological assessment, and scores on Wechsler subtests.Conclusions. An unambiguous conclusion about the violation of speech development in children conceived by IVF cannot be drawn, however, in the presence of mental pathology and taking into account the age of the mother and the number of ART procedures, attention should be paid to the provision of speech therapy and neuropsychological correction from an early age.ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅. ΠΡΡΠΎΠΊΠ°Ρ ΡΠ°ΡΡΠΎΡΠ° ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π²ΡΠΏΠΎΠΌΠΎΠ³Π°ΡΠ΅Π»ΡΠ½ΡΡ
ΡΠ΅ΠΏΡΠΎΠ΄ΡΠΊΡΠΈΠ²Π½ΡΡ
ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ (ΠΠ Π’) ΠΈ ΠΏΡΠΎΡΠΈΠ²ΠΎΡΠ΅ΡΠΈΠ²ΠΎΡΡΡ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΎ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°Ρ
ΠΊΠΎΠ³Π½ΠΈΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π΄Π΅ΡΠ΅ΠΉ, Π·Π°ΡΠ°ΡΡΡ
Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΊΡΡΡΠ°ΠΊΠΎΡΠΏΠΎΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΎΠΏΠ»ΠΎΠ΄ΠΎΡΠ²ΠΎΡΠ΅Π½ΠΈΡ (ΠΠΠ) ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΠ»Π° ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΠΊΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ.Π¦Π΅Π»Ρ ΡΠ°Π±ΠΎΡΡ β ΠΎΡΠ΅Π½ΠΊΠ° ΡΠ²ΠΎΠ΅ΠΎΠ±ΡΠ°Π·ΠΈΡ ΡΠ΅ΡΠ΅Π²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π΄Π΅ΡΠ΅ΠΉ ΠΈ ΠΏΠΎΠ΄ΡΠΎΡΡΠΊΠΎΠ², Π·Π°ΡΠ°ΡΡΡ
Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΏΡΠΎΡΠ΅Π΄ΡΡΡ ΠΠΠ ΠΈ Π½Π°Ρ
ΠΎΠ΄ΡΡΠΈΡ
ΡΡ Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ½ΠΎΠΌ ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π΅ ΠΎΡ 5 Π΄ΠΎ 15 Π»Π΅Ρ.ΠΠ΅ΡΠΎΠ΄Ρ ΠΈ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ. ΠΡΠ±ΠΎΡΠΊΠ° ΠΈΠ· 51 ΡΠ΅Π±Π΅Π½ΠΊΠ° (29 ΠΌΠ°Π»ΡΡΠΈΠΊΠΎΠ²), ΡΡΠ΅Π΄Π½ΠΈΠΉ Π²ΠΎΠ·ΡΠ°ΡΡ β (7,9Β±2,8) Π³ΠΎΠ΄Π°, 14 Π΄Π΅ΡΠ΅ΠΉ ΠΈΠΌΠ΅Π»ΠΈ ΠΏΡΠΈΡ
ΠΈΠ°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π΄ΠΈΠ°Π³Π½ΠΎΠ·Ρ (ΡΠ°ΡΡΡΡΠΎΠΉΡΡΠ²Π° Π°ΡΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΏΠ΅ΠΊΡΡΠ°(Π ΠΠ‘), ΡΠΈΠ·ΠΎΡΠΈΠΏΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ°ΡΡΡΡΠΎΠΉΡΡΠ²ΠΎ (Π¨Π’Π ) ΠΈ Π΄Ρ.). ΠΡΠΈΠΌΠ΅Π½ΡΠ»ΠΈ Π»ΠΎΠ³ΠΎΠΏΠ΅Π΄ΠΈΡΠ΅ΡΠΊΡΡ ΠΎΡΠ΅Π½ΠΊΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠ΅ΡΠΈ, Π½Π΅ΠΉΡΠΎΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΡΡ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΡ ΠΏΠΎ Π.Π‘. Π¦Π²Π΅ΡΠΊΠΎΠ²ΠΎΠΉ, Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΡ IQ ΠΏΠΎ ΠΠ΅ΠΊΡΠ»Π΅ΡΡ, ΠΎΠΏΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ ΡΡΠ°ΡΠΈΡΡΠΈΠΊΡ, ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ·.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π£ 41 % Π΄Π΅ΡΠ΅ΠΉ ΠΈΠΌΠ΅Π»ΠΈΡΡ Π»Π΅Π³ΠΊΠΈΠ΅ Π²Π°ΡΠΈΠ°Π½ΡΡ Π·Π°Π΄Π΅ΡΠΆΠΊΠΈ ΡΠ΅ΡΠ΅Π²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π² Π²ΠΎΠ·ΡΠ°ΡΡΠ΅ Π΄ΠΎ 3 Π»Π΅Ρ, Π½ΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΠΎ ΡΠ°Π·Π²ΠΈΠ²Π°Π»Π°ΡΡ ΡΠ΅ΡΡ Ρ 59 % Π΄Π΅ΡΠ΅ΠΉ. Π‘ Π²ΠΎΠ·ΡΠ°ΡΡΠΎΠΌ ΡΠ°ΡΡΠΎΡΠ° Π²ΡΡΠ²Π»ΡΠ΅ΠΌΡΡ
ΠΎΡΠΊΠ»ΠΎΠ½Π΅Π½ΠΈΠΉ Π² ΡΠ΅ΡΠ΅Π²ΠΎΠΌ ΡΠ°Π·Π²ΠΈΡΠΈΠΈ ΠΏΠ°Π΄Π°Π΅Ρ, Π² ΡΡΠ°ΡΡΠ΅ΠΉ Π²ΠΎΠ·ΡΠ°ΡΡΠ½ΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ (ΠΎΡ 11 Π΄ΠΎ 15 Π»Π΅Ρ) Π½ΠΎΡΠΌΠ° ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠ΅ΡΠΈ Π²ΡΡΡΠ΅ΡΠ°Π»Π°ΡΡ Ρ 85 % ΠΈΡΠΏΡΡΡΠ΅ΠΌΡΡ
. ΠΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΏΠΎΠΊΠ°Π·Π°Π» ΡΠ²ΠΎΠ΅ΠΎΠ±ΡΠ°Π·ΠΈΠ΅ ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΠ»Π΅ΡΠ΄ Ρ Π΄Π΅ΡΠ΅ΠΉ, Π·Π°ΡΠ°ΡΡΡ
Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΠΠ, ΠΏΡΠΈ ΡΠΎΠΏΠΎΡΡΠ°Π²Π»Π΅Π½ΠΈΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ΅ΡΠ΅Π²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ, Π½Π΅ΠΉΡΠΎΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΡΠ΅Π½ΠΊΠΈ, Π±Π°Π»Π»ΠΎΠ² ΠΏΠΎ ΡΡΠ±ΡΠ΅ΡΡΠ°ΠΌ ΠΠ΅ΠΊΡΠ»Π΅ΡΠ°.ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠ΄Π½ΠΎΠ·Π½Π°ΡΠ½ΠΎΠ³ΠΎ Π²ΡΠ²ΠΎΠ΄Π° ΠΎ Π½Π°ΡΡΡΠ΅Π½ΠΈΠΈ ΡΠ΅ΡΠ΅Π²ΠΎΠ³ΠΎ ΡΠ°Π·Π²ΠΈΡΠΈΡ Ρ Π΄Π΅ΡΠ΅ΠΉ, ΡΠΎΠΆΠ΄Π΅Π½Π½ΡΡ
Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΠΠ, ΡΠ΄Π΅Π»Π°ΡΡ Π½Π΅Π»ΡΠ·Ρ, ΠΎΠ΄Π½Π°ΠΊΠΎ ΠΏΡΠΈ Π½Π°Π»ΠΈΡΠΈΠΈ ΠΏΡΠΈΡ
ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ Ρ ΡΡΠ΅ΡΠΎΠΌ Π²ΠΎΠ·ΡΠ°ΡΡΠ° ΠΌΠ°ΡΠ΅ΡΠΈ ΠΈ ΡΠΈΡΠ»Π° ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΏΡΠΎΡΠ΅Π΄ΡΡ ΠΠ Π’ ΡΠ»Π΅Π΄ΡΠ΅Ρ ΠΎΠ±ΡΠ°ΡΠΈΡΡ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° ΠΎΠΊΠ°Π·Π°Π½ΠΈΠ΅ Π»ΠΎΠ³ΠΎΠΏΠ΅Π΄ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ Π½Π΅ΠΉΡΠΎΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΊΠΎΡΡΠ΅ΠΊΡΠΈΠΈ Ρ ΡΠ°Π½Π½Π΅Π³ΠΎ Π²ΠΎΠ·ΡΠ°ΡΡΠ°
Observation Of Very High Energy Cosmic-ray Families In Emulsion Chambers At High Mountain Altitudes (i)
Characteristics of cosmic-ray hadronic interactions in the 1015 - 1017 eV range are studied by observing a total of 429 cosmic-ray families of visible energy greater than 100 TeV found in emulsion chamber experiments at high mountain altitudes, Chacaltaya (5200 m above sea level) and the Pamirs (4300 m above sea level). Extensive comparisons were made with simulated families based on models so far proposed, concentrating on the relation between the observed family flux and the behaviour of high-energy showers in the families, hadronic and electromagnetic components. It is concluded that there must be global change in characteristics of hadronic interactions at around 1016 eV deviating from thise known in the accelerator energy range, specially in the forwardmost angular region of the collision. A detailed study of a new shower phenomenon of small-pT particle emissions, pT being of the order of 10 MeV/c, is carried out and its relation to the origin of huge "halo" phenomena associated with extremely high energy families is discussed as one of the possibilities. General characteristics of such super-families are surveyed. Β© 1992.3702365431Borisov, (1981) Nucl. Phys., 191 BBaybrina, (1984) Trudy FIAN 154, p. 1. , [in Russian], Nauka, MoscowLattes, Hadronic interactions of high energy cosmic-ray observed by emulsion chambers (1980) Physics Reports, 65, p. 151Hasegawa, ICR-Report-151-87-5 (1987) presented at FNAL CDF Seminar, , Inst. for Cosmic Ray Research, Univ. of TokyoCHACALTAYA Emulsion Chamber Experiment (1971) Progress of Theoretical Physics Supplement, 47, p. 1Yamashita, Ohsawa, Chinellato, (1984) Proc. 3rd Int. Symp. on Cosmic Rays and Particle Physics, p. 30. , Tokyo, 1984, Inst. for Cosmic Ray Research, Univ. of Tokyo(1984) Proc. 3rd Int. Symp. on Cosmic Rays and Particle Physics, p. 1. , Tokyo, 1984Baradzei, (1984) Proc. 3rd Int. Symp. on Cosmic Rays and Particle Physics, p. 136. , Tokyo, 1984Yamashita, (1985) J. Phys. Soc. Jpn., 54, p. 529Bolisov, (1984) Proc. 3rd Int. Symp. on Cosmic rays and Particle Physics, p. 248. , Tokyo, 1984, Inst. for Cosmic Ray Research, Univ. of TokyoTamada, Tomaszewski, (1988) Proc. 5th Int. Symp. on Very High Energy Cosmic-Ray Interactions, p. 324. , Lodz, 1988, Inst. for Cosmic Ray Research, Univ. of Tokyo, PolandHasegawa, (1989) ICR-Report-197-89-14, , Inst. for Cosmic Ray Research, Univ. of TokyoCHACALTAYA Emulsion Chamber Experiment (1971) Progress of Theoretical Physics Supplement, 47, p. 1Okamoto, Shibata, (1987) Nucl. Instrum. Methods, 257 A, p. 155Zhdanov, (1980) FIAN preprint no. 45, , Lebedev Physical Institute, MoscowSemba, Gross Features of Nuclear Interactions around 1015eV through Observation of Gamma Ray Families (1983) Progress of Theoretical Physics Supplement, 76, p. 111Nikolsky, (1975) Izv. Akad. Nauk. USSR Ser. Fis., 39, p. 1160Burner, Energy spectra of cosmic rays above 1 TeV per nucleon (1990) The Astrophysical Journal, 349, p. 25Takahashi, (1990) 6th Int. Symp. on Very High Energy Cosmic-ray Interactions, , Tarbes, FranceRen, (1988) Phys. Rev., 38 D, p. 1404Alner, The UA5 high energy simulation program (1987) Nuclear Physics B, 291 B, p. 445Bozzo, Measurement of the proton-antiproton total and elastic cross sections at the CERN SPS collider (1984) Physics Letters B, 147 B, p. 392Wrotniak, (1985) Proc. 19th Cosmic-Ray Conf. La Jolla, 1985, 6, p. 56. , NASA Conference Publication, Washington, D.CWrotniak, (1985) Proc. 19th Cosmic-Ray Conf. La Jolla, 1985, 6, p. 328. , NASA Conference Publication, Washington, D.CMukhamedshin, (1984) Trudy FIAN, 154, p. 142. , Nauka, Moscow, [in Russian]Dunaevsky, Pluta, Slavatinsky, (1988) Proc. 5th Int. Symp. on Very High Energy Cosmic-Ray Interactions, p. 143. , Lodz, 1988, Inst. of Physics, Univ. of Lodz, PolandKaidalov, Ter-Martirosyan, (1987) Proc. 20th Int. Cosmic-Ray Conf., Moscow, 1987, 5, p. 141. , Nauka, MoscowShabelsky, (1985) preprints LNPI-1113Shabelsky, (1986) preprints LNPI-1224, , Leningrad [in Russian]Hillas, (1979) Proc. 16th Int. Cosmic-Ray Conf., Kyoto, 6, p. 13. , Inst. for Cosmic Ray Research, Univ. of TokyoBorisov, (1987) Phys. Lett., 190 B, p. 226Hasegawa, Tamada, (1990) 6th Int. Symp. on Very High Energy Cosmic-Ray Interactions, , Tarbes, FranceSemba, Gross Features of Nuclear Interactions around 1015eV through Observation of Gamma Ray Families (1983) Progress of Theoretical Physics Supplement, p. 111Ren, (1988) Phys. Rev., 38 D, p. 1404Dynaevsky, Zimin, (1988) Proc. 5th Int. Symp. on Very High Energy Cosmic-Ray Interaction, p. 93. , Lodz, 1988, Inst. of Physics, Univ. of Lodz, PolandDynaevsky, (1990) Proc. 6th Int. Symp. on Very High Energy Cosmic-Ray Interactions, , Tarbes, France(1989) FIAN preprint no. 208, , Lebedev Physical Institute, Moscow(1990) Proc. 21st Int. Cosmic-Ray Conf., Adelaide, 8, p. 259. , Dept. Physics and Mathematical Physics, Univ. of Adelaide, AustraliaHasegawa, (1990) ICR-Report-216-90-9, , Inst. for Cosmic-Ray Research, Univ. of TokyoTamada, (1990) Proc. 21st Int. Cosmic-Ray Conf., Adelaide, 1990, 8. , Dept. Physics and Mathematical Physics, Univ. of Adelaide, AustraliaTamada, (1990) ICR-Report-216-90-9(1981) Proc. 17th Int. Cosmic-Ray Conf., Paris, 5, p. 291(1990) Proc. Int. Cosmic-Ray Conf., Adelaide, 1990, 8, p. 267. , Dept. Physics and Mathematical Physics, Univ. of Adelaide, Australia(1989) Inst. Nucl. Phys. 89-67/144, , preprint, Inst. Nucl. Phys., Moscow State UnivSmilnova, (1988) Proc. 5th Int. Sym. on Very High Energy Cosmic-Ray Interactions, p. 42. , Lodz, 1988, Inst. of Physics, Univ. of Lodz, PolandGoulianos, (1986) Proc. Workshop of Particle Simulation at High Energies, , University of Wisconsin, Madison, USAIvanenko, (1983) Proc. 18th Int. Cosmic-Ray Conf., Bangalore, 1983, 5, p. 274. , Tata Inst. Fundamental Research, Bombay, IndiaIvanenko, (1984) Proc. Int. Symp. on Cosmic-Rays and Particle Physics, p. 101. , Tokyo, 1984, Inst. for Cosmic Ray Research, Univ. of Tokyo(1988) 5th Int. Symp. on Very High Energy Cosmic-Ray Interactions, p. 180. , Lodz, 1988, Inst. of Physics, Univ. of Lodz, Poland(1990) Proc. 21st Int. Cosmic-Ray Conf., Adelaide, 1990, 8, p. 251. , Dept. Physics and Mathematical Physics, Univ. of Adelaide, Australia(1991) Izv. AN USSR No. 4, , to be publishedNikolsky, Shaulov, Cherdyntseva, (1990) FIAN preprint no. 140, , Lebedev Physical Institute, Moscow, [in Russian](1987) Proc. 20th Int. Cosmic-Ray Conf., Moscow, 1987, 5, p. 326. , Nauka, Mosco
Formation of Nanostructured Films of Polycrystalline Silicon Doped with Germanium
The impact of germanium as isovalent impurity on the process of formation of nanostructured films of polycrystalline silicon doped with germanium is investigated
Π’Π΅ΡΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΉ Π°Π½Π°Π»ΠΈΠ· ΠΎΡΠ½ΠΎΠ²Π½ΡΡ ΡΠ΅Π°ΠΊΡΠΈΠΉ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉ-ΡΠΈΡΠ°Π½ ΠΏΡΠΈ ΡΠ°ΠΌΠΎΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½ΡΡΡΠ΅ΠΌΡΡ Π²ΡΡΠΎΠΊΠΎΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠΌ ΡΠΈΠ½ΡΠ΅Π·Π΅
Chemical reactions and mechanisms of structure formation in the high-temperature synthesis (SHS) of titanium disilicide are considered. It has been established that the course of exothermic reaction of the silicon-titanium system is determined by the process initiation temperature, the initial nanoscale of powder particles and titanium-to-silicon mass ratio.ΠΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ Π°Π½Π°Π»ΠΈΠ·Π° ΡΠ΅ΡΠΌΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΎΡΠ½ΠΎΠ²Π½ΡΡ
ΡΠ΅Π°ΠΊΡΠΈΠΉ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉ-ΡΠΈΡΠ°Π½ ΠΏΡΠΈ ΡΠ°ΠΌΠΎΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½ΡΡΡΠ΅ΠΌΡΡ Π²ΡΡΠΎΠΊΠΎΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠΌ ΡΠΈΠ½ΡΠ΅Π·Π΅ (Π‘ΠΠ‘) ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½Π° Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ ΡΠΎΠ·Π΄Π°Π½ΠΈΡ Π½Π°Π½ΠΎΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΏΠΎΡΠΎΡΠΊΠΎΠ² Π΄ΠΈΡΠΈΠ»ΠΈΡΠΈΠ΄Π° ΡΠΈΡΠ°Π½Π° (TiSi2) ΠΊΠ°ΠΊ ΠΏΠΎΠ»ΡΠΏΡΠΎΠ²ΠΎΠ΄Π½ΠΈΠΊΠ° Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΡΠ°ΠΌΠΎΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½ΡΡΡΠ΅Π³ΠΎΡΡ Π²ΡΡΠΎΠΊΠΎΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ½ΡΠ΅Π·Π°. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ Ρ
ΠΎΠ΄ ΡΠΊΠ·ΠΎΡΠ΅ΡΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ΅Π°ΠΊΡΠΈΠΉ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ ΠΊΡΠ΅ΠΌΠ½ΠΈΠΉ-ΡΠΈΡΠ°Π½ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΈΠ½ΠΈΡΠΈΠΈΡΡΡΡΠ΅ΠΉ ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠΎΠΉ ΠΏΡΠΎΡΠ΅ΡΡΠ°, ΠΈΡΡ
ΠΎΠ΄Π½ΡΠΌ Π½Π°Π½ΠΎΠΌΠ°ΡΡΡΠ°Π±ΠΎΠΌ ΡΠ°ΡΡΠΈΡ ΠΏΠΎΡΠΎΡΠΊΠΎΠ² ΠΈ ΠΌΠ°ΡΡΠΎΠ²ΡΠΌ ΡΠΎΠΎΡΠ½ΠΎΡΠ΅Π½ΠΈΠ΅ΠΌ ΡΠΈΡΠ°Π½Π° ΠΊ ΠΊΡΠ΅ΠΌΠ½ΠΈΡ
Features of nanoclusters formation in the deposition mode of superthin films SI(GE)
With the use of the scanning, transmission and atomic-force microscopy and Raman scattering of ranges the features of nanoclusters formation of Si, Ge, and solid SiGe solution the deposition mode of superthin films Si(Ge) are studied. The leading mechanism in the process of films crystallization with silicon, germanium and silicongermanium nanostructures alloyed by Ge on all types of initial surfaces of substrates is the migration of silicon and germanium atoms on a surface of films are established. For the self-organization of SiGe nanoclusters a small shift of surface atoms of complex structures on a clean surface with the formation of bonds like GeβGe or SiβSi is favorable. It is caused by the fact that under the thermal treatment the atoms rejected from an ideal position in a crystal grid create additional force fields and it leads to the change of elastic properties of the whole nanocrystal
Investigation of Influence of Cleanliness of the Surface Substrate on Formation and Transformation of Silicon-Germanium Nanoclusters
Established that the degree surface perfection to be seen as an essential part of the
general task of preparing a clean surface before the process of formation of SiGe
nanoclusters and the suppression of their transformation from nanoscale to microsizes. A
small displacement of the surface atoms of complex structures on a clean surface with
the formation of bonds of Ge -Ge or Si- Si is beneficial for self-organization of
nanoclusters SiGe