24 research outputs found
Kinetics of channeling with rechanneling
The basic system of equations of the kinetic theory of channeling with rechanneling is built. A new expression is obtained for channeled fraction taking into account the volume trapping, and rechanneling and dechanneling on rough defects. The existence of new characteristic lengths - the volume trapping length and the rechanneling length - is shown. It is shown, that flux peaking effect modifies the dechanneling cross-sections of the defects.ΠΠΎΠ±ΡΠ΄ΠΎΠ²Π°Π½Π° ΡΠΈΡΡΠ΅ΠΌΠ° ΡΡΠ²Π½ΡΠ½Ρ ΠΊΡΠ½Π΅ΡΠΈΡΠ½ΠΎΡ ΡΠ΅ΠΎΡΡΡ ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ Π· ΠΎΠ±Π»ΡΠΊΠΎΠΌ ΡΠ΅ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ. ΠΡΡΠΈΠΌΠ°Π½ΠΎ Π½ΠΎΠ²Ρ Π²ΠΈΡΠ°ΠΆΠ΅Π½Π½Ρ Π΄Π»Ρ ΡΡΠ½ΠΊΡΡΡ Π΄Π΅ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ Π²ΡΠ°Ρ
ΠΎΠ²ΡΡΡΡ ΠΌΠΎΠΆΠ»ΠΈΠ²ΡΡΡΡ Π΄Π΅ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ, ΠΎΠ±'ΡΠΌΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
ΠΎΠΏΠ»Π΅Π½Π½Ρ Ρ ΡΠ΅ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ Π½Π° ΠΆΠΎΡΡΡΠΊΠΈΡ
Π΄Π΅ΡΠ΅ΠΊΡΠ°Ρ
. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΡΠ½ΡΠ²Π°Π½Π½Ρ Π½ΠΎΠ²ΠΈΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ½ΠΈΡ
Π΄ΠΎΠ²ΠΆΠΈΠ½ Ρ ΠΊΡΠ½Π΅ΡΠΈΡΡ ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ β ΡΠ΅ Π΄ΠΎΠ²ΠΆΠΈΠ½ΠΈ ΡΠ΅ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ ΠΉ ΠΎΠ±'ΡΠΌΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
ΠΎΠΏΠ»Π΅Π½Π½Ρ. Π’Π°ΠΊΠΎΠΆ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΠΎ ΠΎΠ±Π»ΡΠΊ ΡΠΎΠ·ΠΏΠΎΠ΄ΡΠ»Ρ ΡΠ°ΡΡΠΎΠΊ ΠΏΠΎ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΠΈΠΌ ΠΏΠ΅ΡΠ΅ΠΌΡΠ½Π½ΠΈΠΌ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡ Π΄ΠΎ ΠΌΠΎΠ΄ΠΈΡΡΠΊΠ°ΡΡΡ ΠΏΠ΅ΡΠ΅ΡΠΈΠ½Ρ Π΄Π΅ΠΊΠ°Π½Π°Π»ΡΠ²Π°Π½Π½Ρ Π½Π° Π΄Π΅ΡΠ΅ΠΊΡΠ°Ρ
.ΠΠΎΡΡΡΠΎΠ΅Π½Π° ΡΠΈΡΡΠ΅ΠΌΠ° ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΉ ΠΊΠΈΠ½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅ΠΎΡΠΈΠΈ ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Ρ ΡΡΠ΅ΡΠΎΠΌ ΡΠ΅ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠΎΠ»ΡΡΠ΅Π½Ρ Π½ΠΎΠ²ΡΠ΅ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ ΡΡΠ½ΠΊΡΠΈΠΈ Π΄Π΅ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΡΠΈΡΡΠ²Π°ΡΡΠΈΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡ Π΄Π΅ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ, ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
Π²Π°ΡΠ° ΠΈ ΡΠ΅ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π½Π° ΠΆΠ΅ΡΡΠΊΠΈΡ
Π΄Π΅ΡΠ΅ΠΊΡΠ°Ρ
. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΡΡΠ΅ΡΡΠ²ΠΎΠ²Π°Π½ΠΈΠ΅ Π½ΠΎΠ²ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ½ΡΡ
Π΄Π»ΠΈΠ½ Π² ΠΊΠΈΠ½Π΅ΡΠΈΠΊΠ΅ ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ β ΡΡΠΎ Π΄Π»ΠΈΠ½Ρ ΡΠ΅ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΠΎΠ±ΡΠ΅ΠΌΠ½ΠΎΠ³ΠΎ Π·Π°Ρ
Π²Π°ΡΠ°. Π’Π°ΠΊΠΆΠ΅ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, ΡΡΠΎ ΡΡΠ΅Ρ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠ°ΡΡΠΈΡ ΠΏΠΎ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΡΠΌ ΠΏΠ΅ΡΠ΅ΠΌΠ΅Π½Π½ΡΠΌ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡ ΠΊ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π΄Π΅ΠΊΠ°Π½Π°Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π½Π° Π΄Π΅ΡΠ΅ΠΊΡΠ°Ρ
Josephson Coupling through a Quantum Dot
We derive, via fourth order perturbation theory, an expression for the
Josephson current through a gated interacting quantum dot. We analyze our
expression for two different models of the superconductor-dot-superconductor
(SDS) system. When the matrix elements connecting dot and leads are featureless
constants, we compute the Josephson coupling J_c as a function of the gate
voltage and Coulomb interaction. In the diffusive dot limit, we compute the
probability distribution P(J_c) of Josephson couplings. In both cases, pi
junction behavior (J_c < 0) is possible, and is not simply dependent on the
parity of the dot occupancy.Comment: 9 pages; 3 encapsulated PostScript figure
Monitoring of high energy deuteron beams in the experiments with massive targets
The influence of massive uranium target (500 kg natU) of assembly "QUINTA" on the results of high energy deuteron
beam monitoring with aluminum and copper foils was investigated. In order to increase the accuracy of deuteron
beam off-line monitoring, the measurements of the cross sections of fragmentation reaction natCu(d,x)24Na
were performed at 1.32, 2, 4 ΠΈ 8 GeV deuteron energies. For the same deuteron energies the cross sections of residual
nuclei 7
Be, 42K, 52Mn, 57Co and 58Co for natCu(d,x) reaction were measuredΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΠΌΠ°ΡΡΠΈΠ²Π½ΠΎΠΉ ΡΡΠ°Π½ΠΎΠ²ΠΎΠΉ ΠΌΠΈΡΠ΅Π½ΠΈ (500 ΠΊΠ³ natU) ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Β«ΠΠΠΠΠ’ΠΒ» Π½Π° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΡΠΊΠΎΠ² Π΄Π΅ΠΉΡΡΠΎΠ½ΠΎΠ² Ρ ΠΏΠΎΠΌΠΎΡΡΡ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΡΡ
ΠΈ ΠΌΠ΅Π΄Π½ΡΡ
ΡΠΎΠ»ΡΠ³. ΠΠ»Ρ ΡΠ»ΡΡΡΠ΅Π½ΠΈΡ ΡΠΎΡΠ½ΠΎΡΡΠΈ off-line ΠΌΠΎΠ½ΠΈΡΠΎΡΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΡΠΊΠΎΠ² Π΄Π΅ΠΉΡΡΠΎΠ½ΠΎΠ², Π±ΠΎΠΌΠ±Π°ΡΠ΄ΠΈΡΡΡΡΠΈΡ
ΠΏΡΠΎΡΡΠΆΠ΅Π½Π½ΡΠ΅ ΠΌΠΈΡΠ΅Π½ΠΈ ΠΈΠ· ΡΡΠΆΡΠ»ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ², Π±ΡΠ»ΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Ρ ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΡΠ΅ΡΠ΅Π½ΠΈΠΉ ΡΠ΅Π°ΠΊΡΠΈΠΈ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠ°ΡΠΈΠΈ natCu(d,x)24Na Π΄Π»Ρ Π΄Π΅ΠΉΡΡΠΎΠ½ΠΎΠ² Ρ ΡΠ½Π΅ΡΠ³ΠΈΠ΅ΠΉ 1,32; 2; 4 ΠΈ 8 ΠΡΠ. ΠΠ»Ρ ΡΡΠΈΡ
ΠΆΠ΅ ΡΠ½Π΅ΡΠ³ΠΈΠΉ Π΄Π΅ΠΉΡΡΠΎΠ½ΠΎΠ² ΠΈΠ·ΠΌΠ΅ΡΠ΅Π½Ρ ΡΠ΅ΡΠ΅Π½ΠΈΡ Π²ΡΡ
ΠΎΠ΄Π° ΠΈΠ·ΠΎΡΠΎΠΏΠΎΠ² 7 Be, 42K, 52Mn, 57Co ΠΈ 58Co Π² ΡΠ΅Π°ΠΊΡΠΈΡΡ
natCu(d,x).ΠΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½ΠΎ Π²ΠΏΠ»ΠΈΠ² ΠΌΠ°ΡΠΈΠ²Π½ΠΎΡ ΡΡΠ°Π½ΠΎΠ²ΠΎΡ ΠΌΡΡΠ΅Π½Ρ (500 ΠΊΠ³ natU) ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Β«ΠΠΠΠΠ’ΠΒ» Π½Π° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ ΠΌΠΎΠ½ΡΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΏΡΡΠΊΡΠ² Π΄Π΅ΠΉΡΡΠΎΠ½ΡΠ² Π·Π° Π΄ΠΎΠΏΠΎΠΌΠΎΠ³ΠΎΡ Π°Π»ΡΠΌΡΠ½ΡΡΠ²ΠΈΡ
Ρ ΠΌΡΠ΄Π½ΠΈΡ
ΡΠΎΠ»ΡΠ³. ΠΠ»Ρ ΠΏΠΎΠΊΡΠ°ΡΠ΅Π½Π½Ρ ΡΠΎΡΠ½ΠΎΡΡΡ off-line ΠΌΠΎΠ½ΡΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΏΡΡΠΊΡΠ² Π΄Π΅ΠΉΡΡΠΎΠ½ΡΠ², ΡΠΊΡ Π±ΠΎΠΌΠ±Π°ΡΠ΄ΡΡΡΡ ΠΏΡΠΎΡΡΠΆΠ½Ρ ΠΌΡΡΠ΅Π½Ρ Π· Π²Π°ΠΆΠΊΠΈΡ
Π΅Π»Π΅ΠΌΠ΅Π½ΡΡΠ², Π±ΡΠ»ΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½Ρ Π²ΠΈΠΌΡΡΡΠ²Π°Π½Π½Ρ ΠΏΠ΅ΡΠ΅ΡΠΈΠ½ΡΠ² ΡΠ΅Π°ΠΊΡΡΡ ΡΡΠ°Π³ΠΌΠ΅Π½ΡΠ°ΡΡΡ natCu(d,x)24Na Π΄Π»Ρ Π΄Π΅ΠΉΡΡΠΎΠ½ΡΠ² Π· Π΅Π½Π΅ΡΠ³ΡΡΡ 1,32; 2; 4 Ρ 8 ΠΠ΅Π. ΠΠ»Ρ ΡΠΈΡ
ΠΆΠ΅ Π΅Π½Π΅ΡΠ³ΡΠΉ Π΄Π΅ΠΉΡΡΠΎΠ½ΡΠ² Π²ΠΈΠΌΡΡΡΠ½Ρ ΠΏΠ΅ΡΠ΅ΡΠΈΠ½ΠΈ Π²ΠΈΡ
ΠΎΠ΄Ρ ΡΠ·ΠΎΡΠΎΠΏΡΠ² 7 Be, 42K, 52Mn, 57Co Π² ΡΠ΅Π°ΠΊΡΡΡΡ
natCu(d,x)
Periodicities in the Daily Proton Fluxes from 2011 to 2019 Measured by the Alpha Magnetic Spectrometer on the International Space Station from 1 to 100 GV
We present the precision measurement of the daily proton fluxes in cosmic rays from May 20, 2011 to October 29, 2019 (a total of 2824 days or 114 Bartels rotations) in the rigidity interval from 1 to 100 GV based on 5.5Γ109 protons collected with the Alpha Magnetic Spectrometer aboard the International Space Station. The proton fluxes exhibit variations on multiple timescales. From 2014 to 2018, we observed recurrent flux variations with a period of 27 days. Shorter periods of 9 days and 13.5 days are observed in 2016. The strength of all three periodicities changes with time and rigidity. The rigidity dependence of the 27-day periodicity is different from the rigidity dependences of 9-day and 13.5-day periods. Unexpectedly, the strength of 9-day and 13.5-day periodicities increases with increasing rigidities up to βΌ10 GV and βΌ20 GV, respectively. Then the strength of the periodicities decreases with increasing rigidity up to 100 GV.</p
Explicit Digital Models of Linear Complexes
It is obvious that the interoperability of existing digital models is insufficient. Current research on model view definitions and on their semantic enrichment addresses the issue of good interpretation of the results of existing models to improve interoperability. The alternative research presented in this paper is not concerned with interpretation. Instead, the influence of modifications in the geometric and topological concepts of the digital models themselves on their interoperability is investigated. The geometric and topological attributes of the models are made as explicit as possible. Two-dimensional line drawings are replaced by three-dimensional linear complexes to reduce the need for implicit information. The topology of a complex is described with topological tables containing all elements of the model, thus replacing the geometric neighborhood concept of the industry foundation classes. A highly efficient algorithm for the construction of new topological tables of large buildings is presented. The difficulties encountered in modifying existing topological tables are analyzed and solved. Topological and geometric aspects of linear complexes that cannot be treated explicitly with topological tables are identified and presented.Π‘Π»Π΅Π΄ΡΠ΅Ρ ΠΏΡΠΈΠ·Π½Π°ΡΡ, ΡΡΠΎ ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½Π°Ρ ΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΠΎΡΡΡ ΡΠΈΡΡΠΎΠ²ΡΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΡΡ
Π² ΠΏΡΠΎΠ³ΡΠ°ΠΌΠΌΠ½ΡΡ
ΠΏΡΠΎΠ΄ΡΠΊΡΠ°Ρ
ΡΠ°Π·Π½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡΠ΅Π»Π΅ΠΉ, Π½Π° Π΄Π°Π½Π½ΡΠΉ ΠΌΠΎΠΌΠ΅Π½Ρ Π½Π΅ Π΄ΠΎΡΡΠΈΠ³Π½ΡΡΠ°. Π’Π΅ΠΊΡΡΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ Π² ΡΡΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ Π½Π°ΡΠ΅Π»Π΅Π½Ρ Π½Π° ΡΡΠΎΠ²Π΅ΡΡΠ΅Π½ΡΡΠ²ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΈΠ½ΡΠ΅ΡΠΏΡΠ΅ΡΠ°ΡΠΈΠΈ Π΄Π°Π½Π½ΡΡ
ΡΡΡΠ΅ΡΡΠ²ΡΡΡΠΈΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΠΈ ΠΈΡ
ΡΠ΅ΠΌΠ°Π½ΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΎΠ±ΠΎΠ³Π°ΡΠ΅Π½ΠΈΠΈ. ΠΠ»ΡΡΠ΅ΡΠ½Π°ΡΠΈΠ²Π½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅, ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΠΎΠ΅ Π² Π΄Π°Π½Π½ΠΎΠΉ ΡΡΠ°ΡΡΠ΅, ΠΏΠΎΡΠ²ΡΡΠ΅Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΉ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΈ ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΈΠΉ ΡΠ°ΠΌΠΈΡ
ΡΠΈΡΡΠΎΠ²ΡΡ
ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ Π½Π° ΠΈΡ
ΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ ΡΠΎΠ²ΠΌΠ΅ΡΡΠΈΠΌΠΎΡΡΡ. ΠΠ΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°ΡΡΠΈΠ±ΡΡΡ ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ ΡΠ΄Π΅Π»Π°Π½Ρ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΠΎ ΡΠ²Π½ΡΠΌΠΈ. ΠΠ²ΡΠΌΠ΅ΡΠ½ΡΠ΅ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΠ΅ ΡΠ΅ΡΡΠ΅ΠΆΠΈ Π·Π°ΠΌΠ΅Π½ΡΡΡΡΡ ΡΡΠ΅Ρ
ΠΌΠ΅ΡΠ½ΡΠΌΠΈ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΠΌΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ°ΠΌΠΈ, ΡΡΠΎΠ±Ρ ΡΠΌΠ΅Π½ΡΡΠΈΡΡ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎΡΡΡ Π² Π½Π΅ΡΠ²Π½ΠΎΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ. Π’ΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ° ΠΎΠΏΠΈΡΡΠ²Π°Π΅ΡΡΡ ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ°Π±Π»ΠΈΡΠ°ΠΌΠΈ, ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΠΌΠΈ Π²ΡΠ΅ ΡΠ»Π΅ΠΌΠ΅Π½ΡΡ ΠΌΠΎΠ΄Π΅Π»ΠΈ, Π·Π°ΠΌΠ΅Π½ΡΡ, ΡΠ°ΠΊΠΈΠΌ ΠΎΠ±ΡΠ°Π·ΠΎΠΌ, ΠΊΠΎΠ½ΡΠ΅ΠΏΡΠΈΡ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΎΡΠ΅Π΄ΡΡΠ²Π°, ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΠΌΡΡ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ ΠΎΡΡΠ°ΡΠ»Π΅Π²ΡΡ
Π±Π°Π·ΠΎΠ²ΡΡ
ΠΊΠ»Π°ΡΡΠΎΠ² (IFC). ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ Π²ΡΡΠΎΠΊΠΎΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΡΠΉ Π°Π»Π³ΠΎΡΠΈΡΠΌ ΠΏΠΎΡΡΡΠΎΠ΅Π½ΠΈΡ Π½ΠΎΠ²ΡΡ
ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°Π±Π»ΠΈΡ Π±ΠΎΠ»ΡΡΠΈΡ
ΡΡΡΠΎΠΈΡΠ΅Π»ΡΠ½ΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ². ΠΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Ρ ΠΈ ΡΠ΅ΡΠ΅Π½Ρ ΠΏΡΠΎΠ±Π»Π΅ΠΌΡ, Π²ΠΎΠ·Π½ΠΈΠΊΠ°ΡΡΠΈΠ΅ ΠΏΡΠΈ ΠΌΠΎΠ΄ΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΡΡΠ΅ΡΡΠ²ΡΡΡΠΈΡ
ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΡΠ°Π±Π»ΠΈΡ. ΠΡΡΠ²Π»Π΅Π½Ρ ΠΈ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°ΡΠΏΠ΅ΠΊΡΡ Π»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠΎΠ², ΠΊΠΎΡΠΎΡΡΠ΅ Π½Π΅ ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΡΠ²Π½ΠΎ ΠΎΠ±ΡΠ°Π±ΠΎΡΠ°Π½Ρ ΡΠΎΠΏΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ°Π±Π»ΠΈΡΠ°ΠΌΠΈ
Morphology and spectral behavior of hydroxyapatite nanocrystalline coatings obtained by gas detonation deposition
Electronic structure and morphology of hydroxyapatite (HAP), deposited on titanium substrate by gas detonation deposition (GDD), was investigated by scanning probe microscopy of high resolution and spectroscopic methods. Nanoscale structure formation of the coatings in the form of nano-dispersed ceramics was determined. Effects of more advanced surface in the transition of HAP from the crystalline (powder) to nanodispersed (coating) state was studied. It is revealed that the elemental composition of GDD cover surface and subsurface layers remains stable up to the depth of 50 nm. The change of elemental composition of GDD cover subsurface layers in the direction of increasing the calcium and phosphorus content was observed in the range 50-150 nm
The analysis of efficiency of systems of a near radar-location of self-directed antiaircraft guided missiles
Π ΡΡΠ°ΡΡΡ Π²Π²Π΅Π΄Π΅Π½ΠΈΠΉ ΠΊΡΠ»ΡΠΊΡΡΠ½ΠΈΠΉ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊ Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠΈΡΡΠ΅ΠΌ Π±Π»ΠΈΠΆΠ½ΡΠΎΡ ΡΠ°Π΄ΡΠΎΠ»ΠΎΠΊΠ°ΡΡΡ, ΡΠΊΡ Π²ΠΈΠΊΠΎΡΠΈΡΡΠΎΠ²ΡΡΡΡΡΡ Π² ΡΡΠ½ΡΡΡΠΈΡ
ΡΠ°ΠΌΠΎΠ½Π°Π²ΡΠ΄Π½ΠΈΡ
Π·Π΅Π½ΡΡΠ½ΠΈΡ
ΠΊΠ΅ΡΠΎΠ²Π°Π½ΠΈΡ
ΡΠ°ΠΊΠ΅ΡΠ°Ρ
, ΡΠΎ Π΄ΠΎΠ·Π²ΠΎΠ»ΡΡ ΠΎΡΡΠ½ΠΈΡΠΈ ΡΡ
Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡΡΡ. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π°Π½Π°Π»ΡΠ· Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠΈΡΡΠ΅ΠΌ Π±Π»ΠΈΠΆΠ½ΡΠΎΡ ΡΠ°Π΄ΡΠΎΠ»ΠΎΠΊΠ°ΡΡΡ Π² Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ Π²ΡΠ΄ ΡΠΌΠΎΠ² ΠΏΠΎΠ²ΡΡΡΡΠ½ΠΎΡ ΠΎΠ±ΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ (ΠΊΡΡΠ° Π·ΡΡΡΡΡΡΡ ΡΠ°ΠΊΠ΅ΡΠΈ Π· ΡΡΠ»Π»Ρ). ΠΠ° ΠΏΡΠ΄ΡΡΠ°Π²Ρ ΡΡΠΎΠ³ΠΎ Π·ΡΠΎΠ±Π»Π΅Π½ΠΈΠΉ Π²ΠΈΡΠ½ΠΎΠ²ΠΎΠΊ, ΡΠΎ ΠΏΡΠΈ ΠΏΡΠΎΠ΅ΠΊΡΡΠ²Π°Π½Π½Ρ ΡΠΈΡΡΠ΅ΠΌ Π±Π»ΠΈΠΆΠ½ΡΠΎΡ ΡΠ°Π΄ΡΠΎΠ»ΠΎΠΊΠ°ΡΡΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΠΈΡ
Π·Π΅Π½ΡΡΠ½ΠΈΡ
ΠΊΠ΅ΡΠΎΠ²Π°Π½ΠΈΡ
ΡΠ°ΠΊΠ΅Ρ Π½Π΅ΠΎΠ±Ρ
ΡΠ΄Π½ΠΎ ΡΡΠ°Ρ
ΠΎΠ²ΡΠ²Π°ΡΠΈ Π²ΠΏΠ»ΠΈΠ² ΠΊΡΡΠ° Π·ΡΡΡΡΡΡΡ ΡΠ°ΠΊΠ΅ΡΠΈ Π· ΡΡΠ»Π»Ρ Π½Π° Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡΡΡ ΡΠ°ΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ.Π ΡΡΠ°ΡΡΠ΅ Π²Π²Π΅Π΄Π΅Π½ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΠΉ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠΈΡΡΠ΅ΠΌ Π±Π»ΠΈΠΆΠ½Π΅ΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΈ, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΡΡΡΡ Π² ΡΡΡΠ΅ΡΡΠ²ΡΡΡΠΈΡ
ΡΠ°ΠΌΠΎΠ½Π°Π²ΠΎΠ΄ΡΡΠΈΡ
ΡΡ Π·Π΅Π½ΠΈΡΠ½ΡΡ
ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΡΡ
ΡΠ°ΠΊΠ΅ΡΠ°Ρ
, ΡΡΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΎΡΠ΅Π½ΠΈΡΡ ΠΈΡ
ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ. ΠΡΠΎΠ²Π΅Π΄Π΅Π½ Π°Π½Π°Π»ΠΈΠ· ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠΈΡΡΠ΅ΠΌ Π±Π»ΠΈΠΆΠ½Π΅ΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΈ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π²ΠΎΠ·Π΄ΡΡΠ½ΠΎΠΉ ΠΎΠ±ΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ (ΡΠ³Π»Π° Π²ΡΡΡΠ΅ΡΠΈ ΡΠ°ΠΊΠ΅ΡΡ Ρ ΡΠ΅Π»ΡΡ). ΠΠ° ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠΈ ΡΡΠΎΠ³ΠΎ ΡΠ΄Π΅Π»Π°Π½ Π²ΡΠ²ΠΎΠ΄, ΡΡΠΎ ΠΏΡΠΈ ΠΏΡΠΎΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΡΠΈΡΡΠ΅ΠΌ Π±Π»ΠΈΠΆΠ½Π΅ΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΈ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
Π·Π΅Π½ΠΈΡΠ½ΡΡ
ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΡΡ
ΡΠ°ΠΊΠ΅Ρ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ ΡΡΠΈΡΡΠ²Π°ΡΡ Π²Π»ΠΈΡΠ½ΠΈΠ΅ ΡΠ³Π»Π° Π²ΡΡΡΠ΅ΡΠΈ ΡΠ°ΠΊΠ΅ΡΡ Ρ ΡΠ΅Π»ΡΡ Π½Π° ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠ°ΠΊΠΈΡ
ΡΠΈΡΡΠ΅ΠΌ.In article the quantitative index of efficiency of systems of a near radar-location which are used in existing being self-directed antiaircraft guided missiles which allow estimating their efficiency is entered. The analysis of efficiency of systems of a near radarlocation depending on conditions of an air situation (a c orner of a meeting of the rocket and the purpose) is carried out. On the basis of it the conclusion is drawn that at design of systems of a near radar-location of perspective rockets it is necessary to consider influence of a corner of a meeting of the rocket and the purpose on efficiency of such systems