1,613 research outputs found
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΡΠΈΡΡΡΡ Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΡ ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΡΡ Π΄Π»Ρ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ Π²ΡΡΠΎΠΊΠΎΡΠΎΡΠ½ΠΎΠ³ΠΎ Π»ΠΈΡΡΡ
Aerospace, manufacturing, and shipbuilding industries strive to enhance their competitiveness by optimizing material utilization and improving production processes. The investment casting process offers the capability to fabricate intricate and precise components using a diverse range of alloys. However, this method is not without its drawbacks, including high manufacturing costs and a significant rate of defective castings, which can reach up to 30 %. These defects primarily arise from the stresses imposed on the wax patterns and ceramic molds, leading to their distortion. To address this issue, efforts have been made to reduce stress by employing compacted wax powders for the production of investment patterns. However, stress relaxation in the wax patterns remains a concern as it can result in elastic deformation of the compacted material and subsequent alterations in the final product dimensions. To mitigate this issue, a series of tests were conducted with the objective of studying stress relaxation under constant compression strain, as described by the Kohlrausch equation. The obtained results provide valuable insights that enable the prediction of the ultimate dimensions of patterns created using different grades of wax.ΠΠΎΠ½ΠΊΡΡΠ΅Π½ΡΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΠΉ ΠΌΠ°ΡΠΈΠ½ΠΎ-, ΡΡΠ΄ΠΎ- ΠΈ Π°Π²ΠΈΠ°ΡΡΡΠΎΠ΅Π½ΠΈΡ Π²ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΌ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎ- ΠΈ ΡΠ½Π΅ΡΠ³ΠΎΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ, Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π½Π° ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ ΠΈ ΡΠ·Π»ΠΎΠ² Π΄Π΅ΡΠ°Π»Π΅ΠΉ ΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ Π½Π°Π·Π½Π°ΡΠ΅Π½ΠΈΡ. ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π»ΠΈΡΡΡ ΠΏΠΎ Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΠΌ ΠΌΠΎΠ΄Π΅Π»ΡΠΌ (ΠΠΠ) ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π·Π°Π³ΠΎΡΠΎΠ²ΠΎΠΊ ΠΏΠΎΠ²ΡΡΠ΅Π½Π½ΠΎΠΉ ΡΠ°Π·ΠΌΠ΅ΡΠ½ΠΎΠΉ ΠΈ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠ½ΠΎΡΡΠΈ, ΡΠ»ΠΎΠΆΠ½ΠΎΠΉ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠΈ ΠΈΠ· ΡΠΈΡΠΎΠΊΠΎΠΉ Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°ΡΡΡΡ ΡΠΏΠ»Π°Π²ΠΎΠ². Π Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΊΠ°ΠΌ ΠΠΠ ΡΠ»Π΅Π΄ΡΠ΅Ρ ΠΎΡΠ½Π΅ΡΡΠΈ ΠΌΠ½ΠΎΠ³ΠΎΡΡΠ°Π΄ΠΈΠΉΠ½ΠΎΡΡΡ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΈ Π²ΡΡΠΎΠΊΡΡ ΡΡΠΎΠΈΠΌΠΎΡΡΡ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΠ΄ΡΠΊΡΠ°, ΡΡΠΎ ΠΏΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅Ρ Π½Π΅Π΄ΠΎΠΏΡΡΡΠΈΠΌΠΎΡΡΡ Π±ΡΠ°ΠΊΠ°, Π΄ΠΎΠ»Ρ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΠΌΠΎΠΆΠ΅Ρ Π΄ΠΎΡΡΠΈΠ³Π°ΡΡ 30 %. ΠΡΠ°ΠΊ Π² ΠΠΠ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ Π²ΡΠ·Π²Π°Π½ ΡΠ΅ΠΏΠ»ΠΎΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ²Π»Π΅Π½ΠΈΡΠΌΠΈ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°ΡΡΠΈΠΌΠΈ ΡΡΠ΄ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ ΠΈ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»ΠΈΠ²Π°ΡΡΠΈΠΌΠΈ Π½Π°Π»ΠΈΡΠΈΠ΅ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π² ΡΡΡΡΠΊΡΡΡΠ΅ Π²ΠΎΡΠΊΠΎΠΎΠ±ΡΠ°Π·Π½ΡΡ
ΠΈ ΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², ΡΡΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅Ρ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Π² Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΡ
ΠΈ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΎΠ²ΡΡ
ΡΠΎΡΠΌΠ°Ρ
. ΠΠ»Ρ ΡΡΡΡΠ°Π½Π΅Π½ΠΈΡ Π½Π΅Π³Π°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π²Π»ΠΈΡΠ½ΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°ΠΊΡΠΎΡΠ° ΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π² ΡΡΡΡΠΊΡΡΡΠ°Ρ
ΠΏΡΠΎΠΌΠ΅ΠΆΡΡΠΎΡΠ½ΡΡ
ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ ΠΏΡΠΎΡΠ΅ΡΡΠ°, Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΠΎΡΠΌΠΈΡΡΡΡ ΠΏΡΠ΅ΡΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠΎΡΠΎΡΠΊΠΎΠ² Π²ΠΎΡΠΊΠΎΠΎΠ±ΡΠ°Π·Π½ΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΡΡ
ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΉ. ΠΡΠΈ ΡΡΠΎΠΌ Π½Π΅ΡΠ΅ΡΠ΅Π½Π½ΡΠΌ ΠΎΡΡΠ°Π΅ΡΡΡ Π²ΠΎΠΏΡΠΎΡ ΡΠ΅Π»Π°ΠΊΡΠ°ΡΠΈΠΈ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π² ΠΏΡΠ΅ΡΡΠΎΠ²ΠΊΠ°Ρ
, ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡΠΈΡ
ΠΊ ΡΠΏΡΡΠ³ΠΎΠΌΡ ΠΎΡΠΊΠ»ΠΈΠΊΡ ΡΠΏΠ»ΠΎΡΠ½Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° ΠΈ, ΠΊΠ°ΠΊ ΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠ² ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌΠΎΠ³ΠΎ ΠΈΠ·Π΄Π΅Π»ΠΈΡ. ΠΠΎΠΈΡΠΊ Π²Π°ΡΠΈΠ°Π½ΡΠΎΠ² Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠ°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΠΆΠΈΠΌΠ° ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠ΅ΡΡΠΎΠ²ΠΊΠΈ ΠΏΡΠΈΠ²Π΅Π» ΠΊ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠ΅ΡΠΈΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠΎΠ², Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΊΠΎΡΠΎΡΡΡ
ΠΏΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅ΡΡΡ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠ΅Π»Π°ΠΊΡΠ°ΡΠΈΠΈ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Ο Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠΉ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΡΠΆΠ°ΡΠΈΡ, ΠΎΠΏΠΈΡΡΠ²Π°Π΅ΠΌΠΎΠ³ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΠΎΠ»ΡΡΠ°ΡΡΠ°. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ Π² Ρ
ΠΎΠ΄Π΅ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡ ΠΏΡΠΎΠ³Π½ΠΎΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΠΊΠΎΠ½Π΅ΡΠ½ΡΠ΅ ΡΠ°Π·ΠΌΠ΅ΡΡ ΠΏΡΠ΅ΡΡΠΎΠ²ΠΎΠΊ ΠΈ ΡΡΠΎΡΠΌΠΈΡΠΎΠ²Π°ΡΡ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΡΡ ΠΌΠΎΠ΄Π΅Π»Ρ ΠΏΡΠΎΡΠ΅ΡΡΠ°, Π°ΠΊΡΡΠ°Π»ΡΠ½ΡΡ Π΄Π»Ρ ΡΠΈΡΠΎΠΊΠΎΠΉ Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°ΡΡΡΡ Π²ΠΎΡΠΊΠΎΠΎΠ±ΡΠ°Π·Π½ΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΡΡ
Π² ΠΠΠ
Quantal Two-Centre Coulomb Problem treated by means of the Phase-Integral Method I. General Theory
The present paper concerns the derivation of phase-integral quantization
conditions for the two-centre Coulomb problem under the assumption that the two
Coulomb centres are fixed. With this restriction we treat the general
two-centre Coulomb problem according to the phase-integral method, in which one
uses an {\it a priori} unspecified {\it base function}. We consider base
functions containing three unspecified parameters and .
When the absolute value of the magnetic quantum number is not too small, it
is most appropriate to choose . When, on the other hand,
is sufficiently small, it is most appropriate to choose .
Arbitrary-order phase-integral quantization conditions are obtained for these
choices of . The parameters and are determined from the
requirement that the results of the first and the third order of the
phase-integral approximation coincide, which makes the first-order
approximation as good as possible.
In order to make the paper to some extent self-contained, a short review of
the phase-integral method is given in the Appendix.Comment: 23 pages, RevTeX, 4 EPS figures, submitted to J. Math. Phy
FEATURES MODIFYING VARIOUS TYPES OF IRON-CARBON ALLOYS
The article describes the features of the modification of cast iron, high chrome cast iron and steel. It is shown that the modification of cast iron complex modifier should be based on the thickness of the walls of castings, and for steel and high chrome cast iron, it is beneficial to the macro and microstructure. The data confirming the removal of transcrystallization and size reduction microand macrostructure of castings in various types of iron-carbon alloys. Experimentally proved that in the transition from columnar to equiaxed structure observed increase in the number of eutectic cells, which confirms the position that transcrystallization terminated as a result of nucleation and growth of equiaxed crystalsin the area of concentration supercoolin
Neutral and non-neutral collisionless plasma equilibria for twisted flux tubes: the Gold-Hoyle model in a background field
We calculate exact one-dimensional collisionless plasma equilibria for a continuum of flux tube models, for which the total magnetic field is made up of the βforce-freeβ Gold-Hoyle magnetic flux tube embedded in a uniform and anti-parallel background magnetic field. For a sufficiently weak background magnetic field, the axial component of the total magnetic field reverses at some finite radius. The presence of the background magnetic field means that the total system is not exactly force-free, but by reducing its magnitude, the departure from force-free can be made as small as desired. The distribution function for each species is a function of the three constants of motion; namely, the Hamiltonian and the canonical momenta in the axial and azimuthal directions. Poisson's equation and AmpΓ¨re's law are solved exactly, and the solution allows either electrically neutral or non-neutral configurations, depending on the values of the bulk ion and electron flows. These equilibria have possible applications in various solar, space, and astrophysical contexts, as well as in the laboratory
On integrable system on with the second integral quartic in the momenta
We consider integrable system on the sphere with an additional integral
of fourth order in the momenta. At the special values of parameters this system
coincides with the Kowalevski-Goryachev-Chaplygin system.Comment: LaTeX, 6 page
A New Nanoporous Material Based on Amorphous Silicon Dioxide
Processes for making nanoporous SiO2 layers on Si via the irradiation of thermally oxidized silicon wafers with fast ions followed by chemical treatment in a solution or vapor of hydrofluoric acid are presented. It is shown that the density, shape, diameter, and length to diameter ratio of channels etched in silicon dioxide can be controlled by varying the regimes of fast ion irradiation or chemical treatment of SiO2/Si structures. Track parameters calculated using the thermal spike model are compared with the chemical etching data
ΠΡΠ°ΡΠ½ΠΎΠ΅ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΡΠΎΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ°, Π΄Π²ΠΈΠΆΡΡΠ΅Π³ΠΎΡΡ Π² ΠΏΠΎΠ»Π΅ Π²ΡΠ°ΡΠ°ΡΡΠ΅ΠΉΡΡ ΡΠ΅ΡΠ½ΠΎΠΉ Π΄ΡΡΡ
The method of calculation of redshift of light from a point-like source that moves in the gravitational field of the Kerr black hole as a function of time of observation is developed. The widely presented in literature methods for solving the boundary problem are based on a numerical selection of parameters of geodesics. In contrast, the proposed method is based on approximate analytical expressions for isotropic geodesics in the Kerr metric. The proposed method is illustrated by the example of a model problem with parameters corresponding to real stars moving in the immediate vicinity of a supermassive black hole located in the Center of our Galaxy. The same example shows the efficiency and good accuracy of this method.ΠΠ»Ρ ΡΠΎΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΡΠ»Π΅ΠΊΡΡΠΎΠΌΠ°Π³Π½ΠΈΡΠ½ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ, Π΄Π²ΠΈΠΆΡΡΠ΅Π³ΠΎΡΡ Π² Π³ΡΠ°Π²ΠΈΡΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΌ ΠΏΠΎΠ»Π΅ Π²ΡΠ°ΡΠ°ΡΡΠ΅ΠΉΡΡ ΡΠ΅ΡΠ½ΠΎΠΉ Π΄ΡΡΡ, ΠΎΠΏΠΈΡΡΠ²Π°Π΅ΠΌΠΎΠΉ ΠΌΠ΅ΡΡΠΈΠΊΠΎΠΉ ΠΠ΅ΡΡΠ°, ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½ ΠΌΠ΅ΡΠΎΠ΄ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΡ ΠΊΡΠ°ΡΠ½ΠΎΠ³ΠΎ ΡΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΊΠ°ΠΊ ΡΡΠ½ΠΊΡΠΈΠΈ Π²ΡΠ΅ΠΌΠ΅Π½ΠΈ ΡΠ΄Π°Π»Π΅Π½Π½ΠΎΠ³ΠΎ Π½Π°Π±Π»ΡΠ΄Π°ΡΠ΅Π»Ρ. Π ΠΎΡΠ»ΠΈΡΠΈΠ΅ ΠΎΡ ΡΠΈΡΠΎΠΊΠΎ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π² Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ΅ ΡΠΏΠΎΡΠΎΠ±ΠΎΠ², Π³ΡΠ°Π½ΠΈΡΠ½Π°Ρ Π·Π°Π΄Π°ΡΠ° Π΄Π»Ρ ΡΡΠ°Π΅ΠΊΡΠΎΡΠΈΠΈ Π»ΡΡΠ° ΡΠ΅ΡΠ΅Π½Π° Π½Π΅ ΡΠΈΡΠ»Π΅Π½Π½ΡΠΌ ΠΏΠΎΠ΄Π±ΠΎΡΠΎΠΌ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ², Π° Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΏΡΠΈΠ±Π»ΠΈΠΆΠ΅Π½Π½ΡΡ
Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π²ΡΡΠ°ΠΆΠ΅Π½ΠΈΠΉ Π΄Π»Ρ ΠΈΠ·ΠΎΡΡΠΎΠΏΠ½ΡΡ
Π³Π΅ΠΎΠ΄Π΅Π·ΠΈΡΠ΅ΡΠΊΠΈΡ
Π² ΠΌΠ΅ΡΡΠΈΠΊΠ΅ ΠΠ΅ΡΡΠ°. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΡΠΉ ΠΌΠ΅ΡΠΎΠ΄ ΠΏΡΠΎΠΈΠ»Π»ΡΡΡΡΠΈΡΠΎΠ²Π°Π½ Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΠΎΠΉ Π·Π°Π΄Π°ΡΠΈ Ρ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠ°ΠΌΠΈ, ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²ΡΡΡΠΈΠΌΠΈ ΡΠ΅Π°Π»ΡΠ½ΡΠΌ Π·Π²Π΅Π·Π΄Π°ΠΌ, Π΄Π²ΠΈΠΆΡΡΠΈΠΌΡΡ Π² Π½Π΅ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²Π΅Π½Π½ΠΎΠΉ Π±Π»ΠΈΠ·ΠΎΡΡΠΈ ΡΠ²Π΅ΡΡ
ΠΌΠ°ΡΡΠΈΠ²Π½ΠΎΠΉ ΡΠ΅ΡΠ½ΠΎΠΉ Π΄ΡΡΡ, Π½Π°Ρ
ΠΎΠ΄ΡΡΠ΅ΠΉΡΡ Π² ΡΠ΅Π½ΡΡΠ΅ Π½Π°ΡΠ΅ΠΉ ΠΠ°Π»Π°ΠΊΡΠΈΠΊΠΈ. ΠΠ° ΡΡΠΎΠΌ ΠΆΠ΅ ΠΏΡΠΈΠΌΠ΅ΡΠ΅ ΠΏΠΎΠΊΠ°Π·Π°Π½Π° ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈ Ρ
ΠΎΡΠΎΡΠ°Ρ ΡΠΎΡΠ½ΠΎΡΡΡ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π°
Measurement of the Analyzing Power in \\with a Fast Forward --Diproton
A measurement of the analyzing power of the
reaction was carried out at beam energies of 0.5 and 0.8 GeV by detection of a
fast forward proton pair of small excitation energy MeV. The
kinematically complete experiment made use of the ANKE spectrometer at the
internal beam of COSY and a deuterium cluster--jet target. For the first time
the --wave dominance in the fast diproton is experimentally demonstrated in
this reaction. While at GeV the measured analyzing power
vanishes, it reaches almost unity at GeV for neutrons scattered at
. The results are compared with a model taking into
account one--nucleon exchange, single scattering and (1232) excitation
in the intermediate state. The model describes fairly well the unpolarized
cross section obtained earlier by us and the analyzing power at 0.8 GeV, it
fails to reproduce the angular dependence of at 0.5 GeV.Comment: 4 pages, 4 figures, 1 tabl
He Structure and Mechanisms of He Backward Elastic Scattering
The mechanism of He backward elastic scattering is studied.
It is found that the triangle diagrams with the subprocesses He,
He and He, where and
denote the singlet deuteron and diproton pair in the state,
respectively, dominate in the cross section at 0.3-0.8 GeV, and their
contribution is comparable with that for a sequential transfer of a pair
at 1-1.5 GeV.
The contribution of the , estimated on the basis of the spectator
mechanism of the He reaction, increases the HeHe cross section by one order of magnitude as compared to the
contribution of the deuteron alone.
Effects of the initial and final states interaction are taken into account.Comment: 17 pages, Latex, 4 postscript figures, expanded version, accepted by
Physical Review
The Ethnic 'Other' in Ukrainian History Textbooks: The Case of Russia and the Russians
This paper examines portrayals of Russia and the Russians in two generations of Ukrainian history textbooks. It observes that the textbooks are highly condemning of Ukraine's main ethnic other in the guise of foreign ruler: the tsarist authorities and the Soviet regime are always attributed dubious and malicious intentions even if there is appreciation for some of their policies. By contrast, the books, certainly those of the second generation, refrain from presenting highly biased accounts of the ethnic other as a national group (i.e. Russians). Instances where negative judgements do fall onto Russians are counterbalanced by excerpts criticizing ethnic Ukrainians or highlighting conflicting interests within the Ukrainian ethnic group. The negative appraisal of the ethnic other as foreign ruler is clearly instrumental for the nation-building project as it sustains a discourse legitimating the existence of Ukraine as independent state. However, recent trends in history education, the paper concludes, suggest that the importance of nurturing patriotism as a national policy objective is diminishing
- β¦