192 research outputs found
Introduction to TIPS: a theory for creative design
A highly intriguing problem in combining artificial intelligence and engineering design is automation of the creative and innovative phases of the design process. This paper gives a brief introduction to the theory of inventive problem solving (TIPS) selected as a theoretical basis of the authors' research efforts in this field. The research is conducted in the Stevin Project of the Knowledge-Based System Group of the University of Twente (Enschede, The Netherlands) in cooperation with the Invention Machine Laboratory (Minsk, Belarus). This collaboration aims at developing a formal basis for the creation of an automated reasoning system to support creative engineering design
Possible doublet mechanism for a regular component of parity violation in neutron scattering
A nucleus with octupole deformation of the mean field reveals rotational
doublets with the same angular momentum and opposite parity. Mediated by the
Coriolis-type interaction, the doublet structure leads to a strong regular
component in the parity violation caused by weak interaction. This can explain
sign correlations observed in polarized neutron scattering by Th.Comment: 10 pages, revtex, no figure
Effects of T- and P-odd weak nucleon interaction in nuclei: renormalizations due to residual strong interaction, matrix elements between compound states and their correlations with P-violating matrix elements
Manifestations of P-,T-odd weak interaction between nucleons in nucleus are
considered. Renormalization of this interaction due to residual strong
interaction is studied. Mean squared matrix elements of P-,T-odd weak
interaction between compound states are calculated. Correlators between
P-,T-odd and P-odd, T-even weak interaction matrix elements between compound
states are considered and estimates for these quantities are obtained.Comment: Submitted to Phys. Rev. C; 21 pages, REVTEX 3, no figure
The anapole moment and nucleon weak interactions
From the recent measurement of parity nonconservation (PNC) in the Cs atom we
have extracted the constant of the nuclear spin dependent electron-nucleon PNC
interaction, ; the anapole moment constant, ; the strength of the PNC proton-nucleus potential, ; the -meson-nucleon interaction constant,
; and the strength of the neutron-nucleus potential, .Comment: Uses RevTex, 12 pages. We have added an explanation of the effect of
finite nuclear siz
Searches for violation of fundamental time reversal and space reflection symmetries in solid state experiments
The electric dipole moment (EDM) of a particle violates both time reversal
(T) and space reflection (P) symmetries. There have been recent suggestions for
searches of the electron EDM using solid state experiments [1,2]. These
experiments could improve the sensitivity compared to present atomic and
molecular experiments by several orders of magnitude. In the present paper we
calculate the expected effect. We also suggest that this kind of experiment is
sensitive to T,P-violation in nuclear forces and calculate effects caused by
the nuclear Schiff moment.
The compounds under consideration contain magnetic Gd ions and oxygen
O ions. We demonstrate that the main mechanism for the T,P-odd effects
is related to the penetration of the Oxygen 2p-electrons to the Gd core. All
the effects are related to the deformation of the crystal lattice.Comment: 13 pages, 6 figure
Calculation of parity and time invariance violation in the radium atom
Parity (P) and time (T) invariance violating effects in the Ra atom are
strongly enhanced due to close states of opposite parity, the large nuclear
charge Z and the collective nature of P,T-odd nuclear moments. We have
performed calculations of the atomic electric dipole moments (EDM) produced by
the electron EDM and the nuclear magnetic quadrupole and Schiff moments. We
have also calculated the effects of parity non-conservation produced by the
nuclear anapole moment and the weak charge. Our results show that as a rule the
values of these effects are much larger than those considered so far in other
atoms (enhancement is up to 10^5 times).Comment: 18 pages; LaTeX; Submitted to Phys. Rev.
Many Body Correlation Corrections to Superconducting Pairing in Two Dimensions.
We demonstrate that in the strong coupling limit (the superconducting gap
is as large as the chemical potential ), which is relevant to the
high- superconductivity, the correlation corrections to the gap and
critical temperature are about 10\% of the corresponding mean field
approximation values. For the weak coupling () the correlation
corrections are very large: of the order of 100\% of the corresponding mean
field values.Comment: LaTeX 12 page
Electric dipole moments of Hg, Xe, Rn, Ra, Pu, and TlF induced by the nuclear Schiff moment and limits on time-reversal violating interactions
We have calculated the atomic electric dipole moments (EDMs) induced in
^{199}Hg, ^{129}Xe, ^{223}Rn, ^{225}Ra, and ^{239}Pu by their respective
nuclear Schiff moments S. The results are (in units 10^{-17}S(e {fm}^{3})^{-1}e
cm): d(^{199}Hg)=-2.8, d(^{129}Xe)=0.38, d(^{223}Rn)=3.3, d(^{225}Ra)=-8.5,
d(^{239}Pu)=-11. We have also calculated corrections to the parity- and
time-invariance-violating (P,T-odd) spin-axis interaction constant in TlF.
These results are important for the interpretation of atomic and molecular
experiments on EDMs in terms of fundamental P,T-odd parameters.Comment: 16 page
Induced Parity Nonconserving Interaction and Enhancement of Two-Nucleon Parity Nonconserving Forces
Two-nucleon parity nonconserving (PNC) interaction induced by the
single-particle PNC weak potential and the two-nucleon residual strong
interaction is considered. An approximate analytical formula for this Induced
PNC Interaction (IPNCI) between proton and neutron is derived (), and the
interaction constant is estimated. As a result of coherent contributions from
the nucleons to the PNC potential, IPNCI is an order of magnitude stronger
() than the residual weak two-nucleon interaction and has a
different coordinate and isotopic structure (e.g., the strongest part of IPNCI
does not contribute to the PNC mean field). IPNCI plays an important role in
the formation of PNC effects, e.g., in neutron-nucleus reactions. In that case,
it is a technical way to take into account the contribution of the distant
(small) components of a compound state which dominates the result. The absence
of such enhancement () in the case of T- and P-odd interaction
completes the picture.Comment: Phys. Rev. C, to appear; 17 pages, revtex 3, no figure
ΠΠΈΡΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΡΠΉ ΠΎΡΡΠ΅ΠΎΠ³Π΅Π½Π΅Π· ΠΏΡΠΈ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠΌ ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΠΌ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΡΡΠ΅ΡΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΈ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π°: ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅
Background. The methods of βlengthening over the nailβ (LON) and the sequential use of the external fixation and nailing in the option βlengthening and then the nailβ (LATN) are characterized by ignoring non-observance of the formulated by G.A. Ilizarov is the most important condition for optimizing the osteogenesis process, namely, the preservation of medullary blood supply and osteogenic bone marrow tissue. At the same time, in clinical practice, there was no negative effect of the intramedullary nail on the formation of the regenerate. In experimental studies, the activation of periosteal bone formation during LON is noted. But the active periosteal bone formation detected in clinical practice with a sequential technique has not been confirmed by experimental studies.The aim of the study was to compare the organotypical rebuilding of the distraction regenerate during tibial lengthening in rabbits according to Ilizarov, over the intramedullary fixator and with the sequential use of the external fixation and nailing.Materials and Methods. The study was carried out on 54 mature rabbits of the Soviet Chinchilla breed, which were divided into 3 groups of 18 animals. In Gr-1 (control), the tibia was lengthened by 1 cm in a mini-Ilizarov apparatus at a rate of 1 mm per day for 4 sessions step. In Gr-2, the LATN technique was modeled. After the end of lengthening, an intramedullary fixator was implanted installed, the apparatus with the presence of wires only in the base supports was kept as an imitation of blocking the intramedullary fixator. In Gr-3, lengthening was performed over the intramedullary fixator; at the end of lengthening, the wires were left only in the base supports. The fixation period was is 30 days. The total duration of the experiment is 45 days. On the 10th, 15th, 20th, 30th, 45th day X-ray, CT and morphological studies were performed during the experiment.Results. In the experimental groups, a more pronounced periosteal bone formation in the area of regenerates was noted, while in Gr-3 (LON) cortical plates were formed mainly from the periosteal component, and in Gr-2 (LATN) wide cortical plates were formed from the intermediate and periosteal areas. In this group, the maximum densitometric density values are noted. Endosteal bone formation was preserved in all groups.Conclusion. The LON and LATN techniques, when compared with the classical Ilizarov lengthening, do not demonstrate any deficiency in the organotypical rebuilding of the bone tissue of the regenerates. All zones of bone formation are present, including endosteal, with intense periosteal bone formation. The most powerful bone structures are formed with the sequential use of the external fixation and nailing (LATN) in the form of the formation of wide cortical plates due to the intermediate and periosteal zones of the regenerate.ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅. ΠΠ΅ΡΠΎΠ΄Ρ Β«ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ²Π΅ΡΡ
Π³Π²ΠΎΠ·Π΄ΡΒ» (Π£ΠΠ) ΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΡΠ΅ΡΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΈ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π° Π² Π²Π°ΡΠΈΠ°Π½ΡΠ΅ Β«ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠ΅ Π·Π°ΡΠ΅ΠΌ Π³Π²ΠΎΠ·Π΄ΡΒ» (Π£ΠΠ) Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΡΡΡΡΡ Π½Π΅ΡΠΎΠ±Π»ΡΠ΄Π΅Π½ΠΈΠ΅ΠΌ ΡΡΠΎΡΠΌΡΠ»ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ Π.Π. ΠΠ»ΠΈΠ·Π°ΡΠΎΠ²ΡΠΌ Π²Π°ΠΆΠ½Π΅ΠΉΡΠ΅Π³ΠΎ ΡΡΠ»ΠΎΠ²ΠΈΡ ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΎΡΡΠ΅ΠΎΠ³Π΅Π½Π΅Π·Π°, Π° ΠΈΠΌΠ΅Π½Π½ΠΎ β ΡΠΎΡ
ΡΠ°Π½Π΅Π½ΠΈΡ ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΠΊΡΠΎΠ²ΠΎΡΠ½Π°Π±ΠΆΠ΅Π½ΠΈΡ ΠΈ ΠΎΡΡΠ΅ΠΎΠ³Π΅Π½Π½ΠΎΠΉ ΠΊΠΎΡΡΠ½ΠΎΠΌΠΎΠ·Π³ΠΎΠ²ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ. ΠΡΠΈ ΡΡΠΎΠΌ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅ Π½Π΅ ΠΎΡΠΌΠ΅ΡΠ΅Π½ΠΎ Π½Π΅Π³Π°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π²Π»ΠΈΡΠ½ΠΈΡ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΡΡΠ΅ΡΠΆΠ½Ρ Π½Π° ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠ°. Π ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΡΠ°Π±ΠΎΡΠ°Ρ
ΠΎΡΠΌΠ΅ΡΠ°ΡΡ Π°ΠΊΡΠΈΠ²ΠΈΠ·Π°ΡΠΈΡ ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΈ Π£ΠΠ. ΠΡΡΠ²Π»ΡΠ΅ΠΌΠΎΠ΅ Π² ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠ°ΠΊΡΠΈΠΊΠ΅ Π°ΠΊΡΠΈΠ²Π½ΠΎΠ΅ ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΊΠΎΡΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΠΉ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅ Π½Π΅ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½ΠΎ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΠΌΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡΠΌΠΈ.Π¦Π΅Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ β ΡΡΠ°Π²Π½ΠΈΡΡ ΠΎΡΠ³Π°Π½ΠΎΡΠΈΠΏΠΈΡΠ΅ΡΠΊΡΡ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΡ Π΄ΠΈΡΡΡΠ°ΠΊΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠ° ΠΏΡΠΈ ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠΈ Π³ΠΎΠ»Π΅Π½ΠΈ Ρ ΠΊΡΠΎΠ»ΠΈΠΊΠΎΠ² ΠΏΠΎ ΠΠ»ΠΈΠ·Π°ΡΠΎΠ²Ρ, ΠΏΠΎΠ²Π΅ΡΡ
ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠΊΡΠ°ΡΠΎΡΠ° ΠΈ ΠΏΡΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΠΌ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΡΡΠ΅ΡΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΈ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π°.ΠΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π½Π° 54 ΠΏΠΎΠ»ΠΎΠ²ΠΎΠ·ΡΠ΅Π»ΡΡ
ΠΊΡΠΎΠ»ΠΈΠΊΠ°Ρ
ΠΏΠΎΡΠΎΠ΄Ρ Π‘ΠΎΠ²Π΅ΡΡΠΊΠ°Ρ Π¨ΠΈΠ½ΡΠΈΠ»Π»Π°, ΠΊΠΎΡΠΎΡΡΠ΅ Π±ΡΠ»ΠΈ ΡΠ°Π·Π΄Π΅Π»Π΅Π½Ρ Π½Π° 3 Π³ΡΡΠΏΠΏΡ ΠΏΠΎ 18 ΠΎΡΠΎΠ±Π΅ΠΉ. Π ΠΡ-1 (ΠΊΠΎΠ½ΡΡΠΎΠ»ΡΠ½ΠΎΠΉ) ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠ΅ Π³ΠΎΠ»Π΅Π½ΠΈ Π½Π° 1 ΡΠΌ Π² ΠΌΠΈΠ½ΠΈ-Π°ΠΏΠΏΠ°ΡΠ°ΡΠ΅ ΠΠ»ΠΈΠ·Π°ΡΠΎΠ²Π° Π² ΡΠ΅ΠΌΠΏΠ΅ 1 ΠΌΠΌ Π² ΡΡΡΠΊΠΈ Π·Π° 4 ΠΏΡΠΈΠ΅ΠΌΠ°. Π ΠΡ-2 ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π»ΠΈ ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΡ Π£ΠΠ; ΠΏΠΎΡΠ»Π΅ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΡ ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΡ ΡΡΡΠ°Π½Π°Π²Π»ΠΈΠ²Π°Π»ΠΈ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΡΠΉ ΡΠΈΠΊΡΠ°ΡΠΎΡ, Π°ΠΏΠΏΠ°ΡΠ°Ρ Ρ Π½Π°Π»ΠΈΡΠΈΠ΅ΠΌ ΡΠΏΠΈΡ ΡΠΎΠ»ΡΠΊΠΎ Π² Π±Π°Π·ΠΎΠ²ΡΡ
ΠΎΠΏΠΎΡΠ°Ρ
ΡΠΎΡ
ΡΠ°Π½ΡΠ»ΠΈ ΠΊΠ°ΠΊ ΠΈΠΌΠΈΡΠ°ΡΠΈΡ Π±Π»ΠΎΠΊΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠΊΡΠ°ΡΠΎΡΠ°. Π ΠΡ-3 ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ²Π΅ΡΡ
ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠΊΡΠ°ΡΠΎΡΠ°, ΠΏΠΎ ΠΎΠΊΠΎΠ½ΡΠ°Π½ΠΈΠΈ ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΡ ΡΠΏΠΈΡΡ ΠΎΡΡΠ°Π²Π»ΡΠ»ΠΈ ΡΠΎΠ»ΡΠΊΠΎ Π² Π±Π°Π·ΠΎΠ²ΡΡ
ΠΎΠΏΠΎΡΠ°Ρ
. ΠΠ΅ΡΠΈΠΎΠ΄ ΡΠΈΠΊΡΠ°ΡΠΈΠΈ 30 ΡΡΡ. ΠΠ±ΡΠ°Ρ Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΡ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ° 45 ΡΡΡ. ΠΠ° 10-Π΅, 15-Π΅, 20-Π΅, 30-Π΅, 45-Π΅ ΡΡΡ. ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ° Π²ΡΠΏΠΎΠ»Π½ΡΠ»ΠΈ ΡΠ΅Π½ΡΠ³Π΅Π½ΠΎΠ³ΡΠ°ΡΠΈΡ, ΠΠ’ ΠΈ ΠΌΠΎΡΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
Π³ΡΡΠΏΠΏΠ°Ρ
ΠΎΡΠΌΠ΅ΡΠ΅Π½ΠΎ Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ΅ ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΊΠΎΡΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΎΠ², ΠΏΡΠΈ ΡΡΠΎΠΌ Π² ΠΡ-3 ΠΊΠΎΡΡΠΈΠΊΠ°Π»ΡΠ½ΡΠ΅ ΠΏΠ»Π°ΡΡΠΈΠ½ΠΊΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π»ΠΈΡΡ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ ΠΈΠ· ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠ°, Π° Π² ΠΡ-2 ΡΠΈΡΠΎΠΊΠΈΠ΅ ΠΊΠΎΡΡΠΈΠΊΠ°Π»ΡΠ½ΡΠ΅ ΠΏΠ»Π°ΡΡΠΈΠ½ΠΊΠΈ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π»ΠΈΡΡ ΠΈΠ· ΠΈΠ½ΡΠ΅ΡΠΌΠ΅Π΄ΠΈΠ°ΡΠ½ΠΎΠΉ ΠΈ ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠ΅ΠΉ. Π ΡΡΠΎΠΉ Π³ΡΡΠΏΠΏΠ΅ ΠΎΡΠΌΠ΅ΡΠ΅Π½Ρ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΡΠ΅ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΠΈ Π΄Π΅Π½ΡΠΈΡΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠ»ΠΎΡΠ½ΠΎΡΡΠΈ. ΠΠΎ Π²ΡΠ΅Ρ
Π³ΡΡΠΏΠΏΠ°Ρ
ΡΠΎΡ
ΡΠ°Π½ΡΠ»ΠΎΡΡ ΡΠ½Π΄ΠΎΡΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΊΠΎΡΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅.ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. ΠΠ΅ΡΠΎΠ΄ΠΈΠΊΠΈ Π£ΠΠ ΠΈ Π£ΠΠ ΠΏΡΠΈ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠΈ Ρ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΡΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠ΅ΠΌ ΠΏΠΎ ΠΠ»ΠΈΠ·Π°ΡΠΎΠ²Ρ Π½Π΅ Π΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΡΡΡ ΠΊΠ°ΠΊΠΎΠ³ΠΎ-Π»ΠΈΠ±ΠΎ Π΄Π΅ΡΠΈΡΠΈΡΠ° Π² ΠΎΡΠ³Π°Π½ΠΎΡΠΈΠΏΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠ΅ ΠΊΠΎΡΡΠ½ΠΎΠΉ ΡΠΊΠ°Π½ΠΈ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠΎΠ². ΠΡΠΈΡΡΡΡΡΠ²ΡΡΡ Π²ΡΠ΅ Π·ΠΎΠ½Ρ ΠΊΠΎΡΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ, Π²ΠΊΠ»ΡΡΠ°Ρ ΡΠ½Π΄ΠΎΡΡΠ°Π»ΡΠ½ΡΡ, ΠΏΡΠΈ ΡΡΠΎΠΌ ΠΎΡΠΌΠ΅ΡΠ°Π΅ΡΡΡ ΠΈΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΠΎΠ΅ ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΊΠΎΡΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠ΅. ΠΠ°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΌΠΎΡΠ½ΡΠ΅ ΠΊΠΎΡΡΠ½ΡΠ΅ ΡΡΡΡΠΊΡΡΡΡ ΡΠΎΡΠΌΠΈΡΡΡΡΡΡ ΠΏΡΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΠΎΠ²Π°ΡΠ΅Π»ΡΠ½ΠΎΠΌ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΡΡΠ΅ΡΠΊΠΎΡΡΠ½ΠΎΠ³ΠΎ ΠΈ ΠΈΠ½ΡΡΠ°ΠΌΠ΅Π΄ΡΠ»Π»ΡΡΠ½ΠΎΠ³ΠΎ ΠΎΡΡΠ΅ΠΎΡΠΈΠ½ΡΠ΅Π·Π° (Π£ΠΠ) Π² Π²ΠΈΠ΄Π΅ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠΈΡΠΎΠΊΠΈΡ
ΠΊΠΎΡΡΠΈΠΊΠ°Π»ΡΠ½ΡΡ
ΠΏΠ»Π°ΡΡΠΈΠ½ΠΎΠΊ Π·Π° ΡΡΠ΅Ρ ΠΈΠ½ΡΠ΅ΡΠΌΠ΅Π΄ΠΈΠ°ΡΠ½ΠΎΠΉ ΠΈ ΠΏΠ΅ΡΠΈΠΎΡΡΠ°Π»ΡΠ½ΠΎΠΉ Π·ΠΎΠ½ ΡΠ΅Π³Π΅Π½Π΅ΡΠ°ΡΠ°
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