13 research outputs found
Properties uniformity studies for scintillation elements of 1D- and 2D-matrices on the basis of crystals ZnSe(Te), CdWOβ, CsI(Tl), BiβGeβOββ
Results are presented on parameters of light output and uniformity of scintillation properties of 1D and 2D-matrices for different conditions of their preparation. It has been shown that with grinded scintillators based on
ZnSe(Te) and CdWOβ light output is higher as compared with the polished ones. Energy resolution and light output
have been measured for 2D-scintillators on the basis of CdWOβ, CsI(Tl), ZnSe(Te) for Ξ³-radiation and Ξ±-particles
from Β²Β³β΅Pu. Advantages of 2D-scintillators over monolithic scintillators are shown.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² ΡΠ²ΡΡΠ»ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΡ
ΠΎΠ΄Ρ ΠΉ ΠΎΠ΄Π½ΠΎΡΡΠ΄Π½ΠΎΡΡΡ ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΡΠΉΠ½ΠΈΡ
Π²Π»Π°ΡΡΠΈΠ²ΠΎΡΡΠ΅ΠΉ 1D- Ρ 2D-ΠΌΠ°ΡΡΠΈΡΡ Ρ Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ Π²ΡΠ΄ ΡΠΌΠΎΠ² ΡΡ
Π²ΠΈΠ³ΠΎΡΠΎΠ²Π»Π΅Π½Π½Ρ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ Π·Π±ΡΠ»ΡΡΠ΅Π½Π½Ρ ΡΠ²ΡΡΠ»ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΡ
ΠΎΠ΄Ρ ΡΠ»ΡΡΠΎΠ²Π°Π½ΠΈΡ
ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΡΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Ρ ZnSe(Te) Ρ CdWOβ ΡΠΎΠ΄ΠΎ ΠΏΠΎΠ»ΡΡΠΎΠ²Π°Π½ΠΈΡ
Π΅Π»Π΅ΠΌΠ΅Π½ΡΡΠ². ΠΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½ΠΎ Π΅Π½Π΅ΡΠ³Π΅ΡΠΈΡΠ½Π΅ ΡΠΎΠ·Π΄ΡΠ»Π΅Π½Π½Ρ ΡΠ° ΡΠ²ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π²ΠΈΡ
ΡΠ΄ 2D-ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΡΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Ρ ZnSe(Te) Π΄Π»Ρ Ξ±--ΡΠ°ΡΡΠΎΠΊ Β²Β³β΅Pu. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΠΏΠ΅ΡΠ΅Π²Π°Π³Ρ 2D-ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΡΠ² Ρ ΠΏΠΎΡΡΠ²Π½ΡΠ½Π½Ρ Π· ΠΌΠΎΠ½ΠΎΠ»ΡΡΠ½ΠΈΠΌΠΈ ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΠ°ΠΌΠΈ.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ²Π΅ΡΠΎΠ²ΠΎΠ³ΠΎ Π²ΡΡ
ΠΎΠ΄Π° ΠΈ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΡΡΠΈ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ²ΠΎΠΉΡΡΠ² 1D- ΠΈ 2D-ΠΌΠ°ΡΡΠΈΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΈΡ
ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΡΠ²Π΅ΡΠΎΠ²ΡΡ
ΠΎΠ΄Π° ΡΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ZnSe(Te) ΠΈ CdWOβ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΏΠΎΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ². ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ°Π·ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΈ ΡΠ²Π΅ΡΠΎΠ²ΡΡ
ΠΎΠ΄ 2D-ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ZnSe(Te) Π΄Π»Ρ Ξ±-ΡΠ°ΡΡΠΈΡ Β²Β³β΅Pu. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²ΠΎ 2D-ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠΎΠ² ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΌΠΎΠ½ΠΎΠ»ΠΈΡΠ½ΡΠΌΠΈ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠ°ΠΌΠΈ
Asymptotic Flatness, Little String Theory, and Holography
We argue that any non-gravitational holographic dual to asymptotically flat
string theory in -dimensions naturally resides at spacelike infinity. Since
spacelike infinity can be resovled as a -dimensional timelike
hyperboloid (i.e., as a copy of de Sitter space in dimensions), the
dual theory is defined on a Lorentz signature spacetime. Conceptual issues
regarding such a duality are clarified by comparison with linear dilaton
boundary conditions, such as those dual to little string theory. We compute
both time-ordered and Wightman boundary 2-point functions of operators dual to
massive scalar fields in the asymptotically flat bulk.Comment: 27 pages, 2 figures. Explicit discussion added of using the Wightman
function method to calculate time-ordered boundary 2-point functions. The
resulting branch cuts are linked to the bulk spectrum of state
1D- and 2D-matrices scintillation elements on the crystals base ZnSe(Te), CdWOβ, CsI(Tl), BiβGeβOββ
Results are presented of light output and uniformity of scintillation parameters of 1D and 2D-matrices for different conditions of their preparation. It has been shown that with grinded scintillators based on ZnSe(Te) and CdWO4 light output is higher as compared with the polished ones. Energy resolution and light output has been measured for 2D-scintillators on the ZnSe(Te) base for a-particles from 235Pu. Advantages of 2D-scintillators over monolithic scintillators are shown.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΡΠ²Π΅ΡΠΎΠ²ΠΎΠ³ΠΎ Π²ΡΡ
ΠΎΠ΄Π° ΠΈ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΠΎΡΡΠΈ ΡΡΠΈΠ½ΡΠΈΠ»-Π»ΡΡΠΈΠΎΠ½Π½ΡΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² 1D ΠΈ 2'-ΠΌΠ°ΡΡΠΈΡ Π² Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΠΈ ΠΎΡ ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΈΡ
ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΠ΅ ΡΠ²Π΅ΡΠΎΠ²ΡΡ
ΠΎΠ΄Π° ΡΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ZnSe(Te) ΠΈ CdWO4 ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΏΠΎΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ². ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΎ ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΡΠ°Π·ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΈ ΡΠ²Π΅ΡΠΎΠ²ΡΡ
ΠΎΠ΄ 2D ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ZnSe(Te) Π΄Π»Ρ a-ΡΠ°ΡΡΠΈΡ 235Π ΠΈ. ΠΠΎΠΊΠ°Π·Π°Π½Ρ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π° 2D ΠΌΠ°ΡΡΠΈΡ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΌΠΎΠ½ΠΎΠ»ΠΈΡΠ½ΡΠΌΠΈ ΡΡΠΈΠ½ΡΠΈΠ»Π»ΡΡΠΎΡΠ°ΠΌΠΈ.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΡΠ½Ρ ΡΠ²ΡΡΠ»ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΡ
ΠΎΠ΄Ρ ΠΉ ΠΎΠ΄Π½ΠΎΡΡΠ΄Π½ΠΎΡΡΡ ΡΡΠΈΠ½ΡΠΈΠ»-Π»ΡΡΡΠΉΠ½ΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡΠ² 1D Ρ 2D-ΠΌΠ°ΡΡΠΈΡΡ Ρ Π·Π°Π»Π΅ΠΆΠ½ΠΎΡΡΡ Π²ΡΠ΄ ΡΠΌΠΎΠ² ΡΡ
Π²ΠΈΠ³ΠΎΡΠΎΠ²Π»Π΅Π½Π½Ρ. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ Π·Π±ΡΠ»ΡΡΠ΅Π½Π½Ρ ΡΠ²ΡΡΠ»ΠΎΠ²ΠΎΠ³ΠΎ Π²ΠΈΡ
ΠΎΠ΄Ρ ΡΠ»ΡΡΠΎΠ²Π°Π½ΠΈΡ
ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΡΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Ρ ZnSe(Te) i CdWO4 ΡΠΎΠ΄ΠΎ ΠΏΠΎΠ»ΡΡΠΎΠ²Π°Π½ΠΈΡ
Π΅Π»Π΅ΠΌΠ΅Π½ΡΡΠ². ΠΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½ΠΎ Π΅Π½Π΅ΡΠ³Π΅ΡΠΈΡΠ½Π΅ ΡΠΎΠ·Π΄ΡΠ»Π΅Π½Π½Ρ ΡΠ° ΡΠ²ΡΡΠ»ΠΎΠ²ΠΈΠΉ Π²ΠΈΡ
ΡΠ΄ 2D ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΡΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Ρ ZnSe(Te) Π΄Π»Ρ a-ΡΠ°ΡΡΠΎΠΊ 235Π ΠΈ. ΠΠ΅Π»ΠΈΡΠΈΠ½Π° Ra ~ 5 %. ΠΠΎΠΊΠ°Π·Π°Π½ΠΎ ΠΏΠ΅ΡΠ΅Π²Π°Π³Ρ 2D ΠΌΠ°ΡΡΠΈΡΡ Π² ΠΏΠΎΡΡΠ²Π½ΡΠ½Π½Ρ Π· ΠΌΠΎΠ½ΠΎΠ»ΡΡΠ½ΠΈΠΌΠΈ ΡΡΠΈΠ½ΡΠΈΠ»ΡΡΠΎΡΠ°ΠΌΠΈ
Nonwoven polycaprolactone scaffolds for tissue engineering: The choice of the structure and the method of cell seeding
Nonwoven polycaprolactone materials produced by electrospinning are perspective internal prosthetic implants. Seeding these implants with multipotent mesenchymal stromal cells stimulates the replacement of the prosthesis with recipient's own connective tissue. Electrospinning method was used for producing polycaprolactone matrices differing in thickness, pore diameter, fiber size, and biomechanical properties. Labeled cells were seeded on scaffolds in three ways: (1) static, (2) dynamic, and (3) directed flow of the cell suspension generated by capillary action. Cell distribution on the surface and the interior of the scaffolds was studied; the metabolic activity of cells was measured by MTT assay. Static seeding method yielded fully confluence of cells covered the entire scaffold surface, but the cells were located primarily in the upper third of the matrix. Dynamic method proved to be effective only for scaffolds of thickness greater than 500 microns, irrespective of the pore diameter. The third method was effective only for scaffolds with the pore diameter of 20-30 microns, regardless of the material thickness. Resorbable nonwoven polycaprolactone electrospun materials have appropriate biomechanical properties and similar to native tissue matrix structures for internal prosthesis. The choice of the most effective cell seeding method depends on the spatial characteristics - the material thickness, pore diameter, and fibers size, which are determined by the electrospinning conditions
ΠΠ΅ΡΠΊΠ°Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΠΈΠΊΠ°ΠΏΡΠΎΠ»Π°ΠΊΡΠΎΠ½Π° Π΄Π»Ρ ΡΠΊΠ°Π½Π΅Π²ΠΎΠΉ ΠΈΠ½ΠΆΠ΅Π½Π΅ΡΠΈΠΈ: Π²ΡΠ±ΠΎΡ ΡΡΡΡΠΊΡΡΡΡ ΠΈ ΡΠΏΠΎΡΠΎΠ±Π° Π·Π°ΡΠ΅Π»Π΅Π½ΠΈΡ
Nonwoven polycaprolactone materials produced by electrospinning are perspective internal prosthetic implants. Seeding these implants with multipotent mesenchymal stromal cells stimulates the replacement of the prosthesis with recipient's own connective tissue. Electrospinning method was used for producing polycaprolactone matrices differing in thickness, pore diameter, fiber size, and biomechanical properties. Labeled cells were seeded on scaffolds in three ways: (1) static, (2) dynamic, and (3) directed flow of the cell suspension generated by capillary action. Cell distribution on the surface and the interior of the scaffolds was studied; the metabolic activity of cells was measured by MTT assay. Static seeding method yielded fully confluence of cells covered the entire scaffold surface, but the cells were located primarily in the upper third of the matrix. Dynamic method proved to be effective only for scaffolds of thickness greater than 500 microns, irrespective of the pore diameter. The third method was effective only for scaffolds with the pore diameter of 20-30 microns, regardless of the material thickness. Resorbable nonwoven polycaprolactone electrospun materials have appropriate biomechanical properties and similar to native tissue matrix structures for internal prosthesis. The choice of the most effective cell seeding method depends on the spatial characteristics - the material thickness, pore diameter, and fibers size, which are determined by the electrospinning conditions.ΠΠ΅ΡΠΊΠ°Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΠΈΠΊΠ°ΠΏΡΠΎΠ»Π°ΠΊΡΠΎΠ½Π°, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΡΠΎΡΠΌΠΎΠ²Π°Π½ΠΈΡ, ΡΠ²Π»ΡΡΡΡΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΠΌΠΈ ΠΈΠΌΠΏΠ»Π°Π½ΡΠ°ΡΠ°ΠΌΠΈ Π΄Π»Ρ ΡΠ½Π΄ΠΎΠΏΡΠΎΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠ°ΡΠ΅Π»Π΅Π½ΠΈΠ΅ ΡΠ°ΠΊΠΈΡ
ΠΈΠΌΠΏΠ»Π°Π½ΡΠ°ΡΠΎΠ² ΠΌΡΠ»ΡΡΠΈΠΏΠΎΡΠ΅Π½ΡΠ½ΡΠΌΠΈ ΠΌΠ΅Π·Π΅Π½Ρ
ΠΈΠΌΠ°Π»ΡΠ½ΡΠΌΠΈ ΡΡΡΠΎΠΌΠ°Π»ΡΠ½ΡΠΌΠΈ ΠΊΠ»Π΅ΡΠΊΠ°ΠΌΠΈ ΡΠΏΠΎΡΠΎΠ±ΡΡΠ²ΡΠ΅Ρ Π·Π°ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΡΠ΅Π·Π° ΡΠΎΠ±ΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΡΠΎΠ΅Π΄ΠΈΠ½ΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΡΡ ΡΠ΅ΡΠΈΠΏΠΈΠ΅Π½ΡΠ°. Π¦Π΅Π»ΡΡ Π½Π°ΡΡΠΎΡΡΠ΅Π³ΠΎ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ²Π»ΡΠ»ΠΎΡΡ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΡΠ΅Ρ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² Π·Π°ΡΠ΅Π»Π΅Π½ΠΈΡ ΠΊΠ»Π΅ΡΠΊΠ°ΠΌΠΈ Π½Π΅ΡΠΊΠ°Π½ΡΡ
Π½ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎΠ»ΠΈΠΊΠ°ΠΏΡΠΎΠ»Π°ΠΊΡΠΎΠ½Π°, ΠΎΠ±Π»Π°Π΄Π°ΡΡΠΈΡ
ΡΠ°Π·Π»ΠΈΡΠ½ΡΠΌΠΈ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΡΠΌΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌΠΈ. ΠΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΡΠΎΡΠΌΠΎΠ²Π°Π½ΠΈΡ Π±ΡΠ»ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ ΡΡΠΈ ΠΎΠ±ΡΠ°Π·ΡΠ° ΠΏΠΎΠ»ΠΈΠΊΠ°ΠΏΡΠΎΠ»Π°ΠΊΡΠΎΠ½ΠΎΠ²ΡΡ
ΠΌΠ°ΡΡΠΈΡ, ΠΎΡΠ»ΠΈΡΠ°ΡΡΠΈΡ
ΡΡ ΡΠΎΠ»ΡΠΈΠ½ΠΎΠΉ, Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠΎΠΌ ΠΏΠΎΡ ΠΈ Π²ΠΎΠ»ΠΎΠΊΠΎΠ½, Π±ΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ. ΠΠ°ΡΠ΅Π»Π΅Π½ΠΈΠ΅ Π½ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ ΠΌΠ΅ΡΠ΅Π½ΡΠΌΠΈ ΠΌΡΠ»ΡΡΠΈΠΏΠΎΡΠ΅Π½ΡΠ½ΡΠΌΠΈ ΠΌΠ΅Π·Π΅Π½Ρ
ΠΈΠΌΠ°Π»ΡΠ½ΡΠΌΠΈ ΡΡΡΠΎΠΌΠ°Π»ΡΠ½ΡΠΌΠΈ ΠΊΠ»Π΅ΡΠΊΠ°ΠΌΠΈ ΠΏΡΠΏΠΎΡΠ½ΠΎΠ³ΠΎ ΠΊΠ°Π½Π°ΡΠΈΠΊΠ° ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΡΡΠ΅ΠΌΡ ΡΠΏΠΎΡΠΎΠ±Π°ΠΌΠΈ: ΡΡΠ°ΡΠΈΡΠ½ΡΠΌ, Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΊΠ°ΠΏΠΈΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΡΡΡΠ΅ΠΊΡΠ°. ΠΡΠ΅Π½ΠΈΠ²Π°Π»ΠΈ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΊΠ»Π΅ΡΠΎΠΊ ΠΏΠΎ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΈ ΡΠΎΠ»ΡΠΈΠ½Π΅ ΠΎΠ±ΡΠ°Π·ΡΠΎΠ², ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΡΠ΅ΡΠΊΡΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΊΠ»Π΅ΡΠΎΠΊ ΠΈΠ·ΠΌΠ΅ΡΡΠ»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΠ’Π’-ΡΠ΅ΡΡΠ°. Π‘ΡΠ°ΡΠΈΡΠ½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΠ» ΠΏΠΎΠ»ΡΡΠΈΡΡ Π½ΠΎΡΠΈΡΠ΅Π»ΠΈ Ρ ΡΠ°Π²Π½ΠΎΠΌΠ΅ΡΠ½ΡΠΌ ΠΏΠΎΠΊΡΡΡΠΈΠ΅ΠΌ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ, ΠΎΠ΄Π½Π°ΠΊΠΎ ΠΊΠ»Π΅ΡΠΊΠΈ Π² ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΌ ΡΠ°ΡΠΏΠΎΠ»Π°Π³Π°Π»ΠΈΡΡ Π² Π²Π΅ΡΡ
Π½Π΅ΠΉ ΡΡΠ΅ΡΠΈ ΠΌΠ°ΡΡΠΈΠΊΡΠ°. ΠΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΎΠΊΠ°Π·Π°Π»ΡΡ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π΅Π½ ΡΠΎΠ»ΡΠΊΠΎ Π΄Π»Ρ Π½ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ ΡΠΎΠ»ΡΠΈΠ½ΠΎΠΉ Π±ΠΎΠ»Π΅Π΅ 500 ΠΌΠΊΠΌ, Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΠΎ ΠΎΡ Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠ° ΠΏΠΎΡ. ΠΠ΅ΡΠΎΠ΄ Π·Π°ΡΠ΅Π»Π΅Π½ΠΈΡ Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΊΠ°ΠΏΠΈΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΡΡΡΠ΅ΠΊΡΠ° Π±ΡΠ» ΡΡΡΠ΅ΠΊΡΠΈΠ²Π΅Π½ ΡΠΎΠ»ΡΠΊΠΎ Π΄Π»Ρ Π½ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ Ρ Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠΎΠΌ ΠΏΠΎΡ 20-30 ΠΌΠΊΠΌ, Π½Π΅Π·Π°Π²ΠΈΡΠΈΠΌΠΎ ΠΎΡ ΡΠΎΠ»ΡΠΈΠ½Ρ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π°. ΠΠΈΠΎΡΠ΅Π·ΠΎΡΠ±ΠΈΡΡΠ΅ΠΌΡΠ΅ Π½Π΅ΡΠΊΠ°Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΠΎ-Π»ΠΈΠΊΠ°ΠΏΡΠΎΠ»Π°ΠΊΡΠΎΠ½Π°, ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ ΡΠ»Π΅ΠΊΡΡΠΎΡΠΎΡΠΌΠΎΠ²Π°Π½ΠΈΡ, ΠΎΠ±Π»Π°Π΄Π°ΡΡ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄ΡΡΠΈΠΌΠΈ Π±ΠΈΠΎΠΌΠ΅Ρ
Π°Π½ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ²ΠΎΠΉΡΡΠ²Π°ΠΌΠΈ Π΄Π»Ρ Π²ΡΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΠΏΠ»Π°ΡΡΠΈΠΊΠΈ Π΄Π΅ΡΠ΅ΠΊΡΠΎΠ² ΡΡΠ΅Π½ΠΎΠΊ Π±ΡΡΡΠ½ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠΈ, ΠΈΠΌΠ΅ΡΡ ΡΡ
ΠΎΠ΄Π½ΠΎΠ΅ Ρ ΠΌΠ°ΡΡΠΈΠΊΡΠΎΠΌ Π½Π°ΡΠΈΠ²Π½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ ΡΡΡΠΎΠ΅Π½ΠΈΠ΅. ΠΡΠ±ΠΎΡ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π° Π·Π°ΡΠ΅Π»Π΅Π½ΠΈΡ Π½ΠΎΡΠΈΡΠ΅Π»Π΅ΠΉ ΠΊΠ»Π΅ΡΠΊΠ°ΠΌΠΈ Π·Π°Π²ΠΈΡΠΈΡ ΠΎΡ Π΅Π³ΠΎ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΡΡ
Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊ - ΡΠΎΠ»ΡΠΈΠ½Ρ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π°, Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠ° ΠΏΠΎΡ ΠΈ Π²ΠΎΠ»ΠΎΠΊΠΎΠ½, ΠΊΠΎΡΠΎΡΡΠ΅, Π² ΡΠ²ΠΎΡ ΠΎΡΠ΅ΡΠ΅Π΄Ρ, ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΡΡΡΡ ΡΡΠ»ΠΎΠ²ΠΈΡΠΌΠΈ ΡΠ»Π΅ΠΊΡΡΠΎΡΠΎΡΠΌΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π°