301 research outputs found
Linear, diatomic crystal: single-electron states and large-radius excitons
The large-radius exciton spectrum in a linear crystal with two atoms in the
unit cell was obtained using the single-electron eigenfunctions and the band
structure, which were found by the zero-range potential (ZRP) method. The
ground-state exciton binding energies for the crystal in vacuum appeared to be
larger than the corresponding energy gaps for any set of the crystal
parameters.Comment: 9 pages, 1 figure, 1 tabl
Π‘ΡΡΠ°ΡΠ½Ρ Π½Π°ΠΏΡΡΠΌΠΊΠΈ ΡΡΠ²ΠΎΡΠ΅Π½Π½Ρ ΡΠ° ΡΠ΄ΠΎΡΠΊΠΎΠ½Π°Π»Π΅Π½Π½Ρ ΠΏΡΠΎΠ±ΡΠΎΡΠΈΠΊΡΠ²
The article describes the topical areas of improvement of probiotics, such as: study of the physiology of promising industrial strains in order to select nutrient media for their cultivation; Β determination of sorption processes of probiotic bacteria as a general biological process; study of the role of metabolic products and biologically active substances of microbial cells to define the nature of the adhesins and the mechanism of antagonistic activity; development of technology for the manufacture of complex products based on consortia of bacteria with a wide spectrum of antagonistic activity; research and synergistic inhibitory effects of various species and strains of probiotic bacteria; improved methods of control of antagonistic activity of preparations containing viable microbial cells and the development of methods for the determination of living organisms and the development of drugs for the correction of the intestinal microflora is not only, but also other open cavities of the human body.Π‘ΡΠ°ΡΡΡ ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π° Π°ΠΊΡΡΠ°Π»ΡΠ½ΡΠΌ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡΠΌ ΡΡΠΎΠ²Π΅ΡΡΠ΅Π½ΡΡΠ²ΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠΎΠ±ΠΈΠΎΡΠΈΠΊΠΎΠ², ΡΠ°ΠΊΠΈΠΌ ΠΊΠ°ΠΊ:Β ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΡΡ
ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π΅Π½Π½ΡΡ
ΡΡΠ°ΠΌΠΌΠΎΠ² Π±Π°ΠΊΡΠ΅ΡΠΈΠΉ Ρ ΡΠ΅Π»ΡΡ ΠΏΠΎΠ΄Π±ΠΎΡΠ° ΠΏΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΡΡ
ΡΡΠ΅Π΄ Π΄Π»Ρ ΠΈΡ
ΠΊΡΠ»ΡΡΠΈΠ²ΠΈΡΠΎΠ²Π°Π½ΠΈΡ;Β ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΡΠΎΡΠ±ΡΠΈΠΈ ΠΏΡΠΎΠ±ΠΈΠΎΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π±Π°ΠΊΡΠ΅ΡΠΈΠΉ ΠΊΠ°ΠΊ ΠΎΠ±ΡΠ΅Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡΠ°;Β ΠΈΠ·ΡΡΠ΅Π½ΠΈΠ΅ ΡΠΎΠ»ΠΈ ΠΏΡΠΎΠ΄ΡΠΊΡΠΎΠ² ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΠΈΠ·ΠΌΠ° ΠΈ ΠΠΠ ΠΌΠΈΠΊΡΠΎΠ±Π½ΠΎΠΉ ΠΊΠ»Π΅ΡΠΊΠΈ Π΄Π»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ ΠΏΡΠΈΡΠΎΠ΄Ρ Π°Π΄Π³Π΅Π·ΠΈΠ½ΠΎΠ² ΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠ° Π°Π½ΡΠ°Π³ΠΎΠ½ΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ; Β ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΡΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Π΅ ΠΊΠΎΠ½ΡΠΎΡΡΠΈΡΠΌΠΎΠ² Π±Π°ΠΊΡΠ΅ΡΠΈΠΉ Ρ ΡΠΈΡΠΎΠΊΠΈΠΌ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌ Π°Π½ΡΠ°Π³ΠΎΠ½ΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ;Β ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠΈΠ½Π΅ΡΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΈ ΠΈΠ½Π³ΠΈΠ±ΠΈΡΠΎΡΠ½ΠΎΠ³ΠΎ Π΄Π΅ΠΉΡΡΠ²ΠΈΡ ΡΠ°Π·Π½ΡΡ
Π²ΠΈΠ΄ΠΎΠ² ΠΈ ΡΡΠ°ΠΌΠΌΠΎΠ² ΠΏΡΠΎΠ±ΠΈΠΎΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π±Π°ΠΊΡΠ΅ΡΠΈΠΉ;Β ΡΡΠΎΠ²Π΅ΡΡΠ΅Π½ΡΡΠ²ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ Π°Π½ΡΠ°Π³ΠΎΠ½ΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ², Β ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠΎΠ΄Π΅ΡΠΆΠ°Ρ ΠΆΠΈΠ·Π½Π΅ΡΠΏΠΎΡΠΎΠ±Π½ΡΠ΅Β ΠΌΠΈΠΊΡΠΎΠ±Π½ΡΠ΅ ΠΊΠ»Π΅ΡΠΊΠΈ ΠΈ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΈΡ
ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ;Β ΡΠΎΠ·Π΄Π°Π½ΠΈΠ΅ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠΎΠ² Π΄Π»Ρ ΠΊΠΎΡΡΠ΅ΠΊΡΠΈΠΈ ΠΌΠΈΠΊΡΠΎΡΠ»ΠΎΡΡ Π½Π΅ ΡΠΎΠ»ΡΠΊΠΎ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΠ°, Π½ΠΎ ΠΈ Π΄ΡΡΠ³ΠΈΡ
ΠΎΡΠΊΡΡΡΡΡ
ΠΏΠΎΠ»ΠΎΡΡΠ΅ΠΉ ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠ° ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ°.Β Π‘ΡΠ°ΡΡΡ ΠΏΡΠΈΡΠ²ΡΡΠ΅Π½Π° Π°ΠΊΡΡΠ°Π»ΡΠ½ΠΈΠΌ Π½Π°ΠΏΡΡΠΌΠΊΠ°ΠΌ ΡΠ΄ΠΎΡΠΊΠΎΠ½Π°Π»Π΅Π½Π½Ρ ΠΏΡΠΎΠ±ΡΠΎΡΠΈΠΊΡΠ², ΡΠ°ΠΊΠΈΠΌ ΡΠΊ:Β Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Π½Ρ ΡΡΠ·ΡΠΎΠ»ΠΎΠ³ΡΡ ΠΏΠ΅ΡΡΠΏΠ΅ΠΊΡΠΈΠ²Π½ΠΈΡ
Π²ΠΈΡΠΎΠ±Π½ΠΈΡΠΈΡ
ΡΡΠ°ΠΌΡΠ² Π· ΠΌΠ΅ΡΠΎΡ ΠΏΡΠ΄Π±ΠΎΡΡ ΠΏΠΎΠΆΠΈΠ²Π½ΠΈΡ
ΡΠ΅ΡΠ΅Π΄ΠΎΠ²ΠΈΡ Π΄Π»Ρ ΡΡ
ΠΊΡΠ»ΡΡΠΈΠ²ΡΠ²Π°Π½Π½Ρ;Β Π²ΠΈΠ·Π½Π°ΡΠ΅Π½Π½Ρ ΠΏΡΠΎΡΠ΅ΡΡΠ² ΡΠΎΡΠ±ΡΡΡ ΠΏΡΠΎΠ±ΡΠΎΡΠΈΡΠ½ΠΈΡ
Π±Π°ΠΊΡΠ΅ΡΡΠΉ ΡΠΊ Π·Π°Π³Π°Π»ΡΠ½ΠΎΠ±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΡΠ΅ΡΡ;Β Π²ΠΈΠ²ΡΠ΅Π½Π½Ρ ΡΠΎΠ»Ρ ΠΏΡΠΎΠ΄ΡΠΊΡΡΠ² ΠΌΠ΅ΡΠ°Π±ΠΎΠ»ΡΠ·ΠΌΡ ΡΠ° Π±ΡΠΎΠ»ΠΎΠ³ΡΡΠ½ΠΎ Π°ΠΊΡΠΈΠ²Π½ΠΈΡ
ΡΠ΅ΡΠΎΠ²ΠΈΠ½ ΠΌΡΠΊΡΠΎΠ±Π½ΠΎΡ ΠΊΠ»ΡΡΠΈΠ½ΠΈ Π΄Π»Ρ Π²ΠΈΠ·Π½Π°ΡΠ΅Π½Π½Ρ ΠΏΡΠΈΡΠΎΠ΄ΠΈ Π°Π΄Π³Π΅Π·ΠΈΠ½ΡΠ² Ρ ΠΌΠ΅Ρ
Π°Π½ΡΠ·ΠΌΡ Π°Π½ΡΠ°Π³ΠΎΠ½ΡΡΡΠΈΡΠ½ΠΎΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ; Β ΡΠΎΠ·ΡΠΎΠ±ΠΊΠ° ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΡΡ Π²ΠΈΠ³ΠΎΡΠΎΠ²Π»Π΅Π½Π½Ρ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΈΡ
ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΡΠ² Π½Π° ΠΎΡΠ½ΠΎΠ²Ρ ΠΊΠΎΠ½ΡΠΎΡΡΡΡΠΌΡΠ² Π±Π°ΠΊΡΠ΅ΡΡΠΉ Π· ΡΠΈΡΠΎΠΊΠΈΠΌ ΡΠΏΠ΅ΠΊΡΡΠΎΠΌ Π°Π½ΡΠ°Π³ΠΎΠ½ΡΡΡΠΈΡΠ½ΠΎΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ;Β Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Π½Ρ ΡΠΈΠ½Π΅ΡΠ³ΡΡΠ½ΠΎΡ ΡΠ° ΡΠ½Π³ΡΠ±ΡΡΠΎΡΠ½ΠΎΡ Π΄ΡΡ ΡΡΠ·Π½ΠΈΡ
Π²ΠΈΠ΄ΡΠ² ΡΠ° ΡΡΠ°ΠΌΡΠ² ΠΏΡΠΎΠ±ΡΠΎΡΠΈΡΠ½ΠΈΡ
Π±Π°ΠΊΡΠ΅ΡΡΠΉ;Β Π²Π΄ΠΎΡΠΊΠΎΠ½Π°Π»Π΅Π½Π½Ρ ΠΌΠ΅ΡΠΎΠ΄ΡΠ² ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ Π°Π½ΡΠ°Π³ΠΎΠ½ΡΡΡΠΈΡΠ½ΠΎΡ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΡΠ², ΡΠΎ ΠΌΡΡΡΡΡΡ ΠΆΠΈΡΡΡΠ·Π΄Π°ΡΠ½Ρ ΠΌΡΠΊΡΠΎΠ±Π½Ρ ΠΊΠ»ΡΡΠΈΠ½ΠΈ ΡΠ° ΡΠΎΠ·ΡΠΎΠ±ΠΊΠ° ΠΌΠ΅ΡΠΎΠ΄ΡΠ² Π²ΠΈΠ·Π½Π°ΡΠ΅Π½Π½Ρ Π²ΠΌΡΡΡΡ ΠΆΠΈΠ²ΠΈΡ
ΠΌΡΠΊΡΠΎΠΎΡΠ³Π°Π½ΡΠ·ΠΌΡΠ²;Β ΡΠΎΠ·ΡΠΎΠ±ΠΊΠ° ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΡΠ² Π΄Π»Ρ ΠΊΠΎΡΠ΅ΠΊΡΡΡ ΠΌΡΠΊΡΠΎΡΠ»ΠΎΡΠΈ Π½Π΅ Π»ΠΈΡΠ΅ ΠΊΠΈΡΠ΅ΡΠ½ΠΈΠΊΡ, Π° ΠΉ ΡΠ½ΡΠΈΡ
Π²ΡΠ΄ΠΊΡΠΈΡΠΈΡ
ΠΏΠΎΡΠΎΠΆΠ½ΠΈΠ½ ΠΎΡΠ³Π°Π½ΡΠ·ΠΌΡ Π»ΡΠ΄ΠΈΠ½ΠΈ.
One-electron states and interband optical absorption in single-wall carbon nanotubes
Explicit expressions for the wave functions and dispersion equation for the
band p - electrons in single-wall carbon nanotubes are obtained within the
method of zero-range potentials. They are then used to investigate the
absorption spectrum of polarized light caused by direct interband transitions
in isolated nanotubes. It is shown that, at least, under the above
approximations, the circular dichroism is absent in chiral nanotubes for the
light wave propagating along the tube axis. The results obtained are compared
with those calculated in a similar way for a graphite plane.Comment: 16 pages, 8 figures, 1 tabl
Spatially and polarization resolved plasmon mediated transmission through continuous metal films
The experimental demonstration and characterization is made of the
plasmon-mediated resonant transmission through an embedded undulated continuous
thin metal film under normal incidence. 1D undulations are shown to enable a
spatially resolved polarisation filtering whereas 2D undulations lead to
spatially resolved, polarization independent transmission. Whereas the needed
submicron microstructure lends itself in principle to CD-like low-cost mass
replication by means of injection moulding and embossing, the present paper
demonstrates the expected transmission effects on experimental models based on
metal-coated photoresist gratings. The spectral and angular dependence in the
neighbourhood of resonance are investigated and the question of the excess
losses exhibited by surface plasmons is discusse
ΠΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡΡΡ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ Π³ΡΠ±ΡΠΈΠ΄Π½ΠΈΡ ΠΏΠΎΡΠΎΡΡΡ Π· ΡΡΠ·Π½ΠΎΡ ΠΌΠ°ΡΠΎΡ ΠΏΡΠΈ ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΡΡ Π·Π° ΡΡΠ΄ΠΊΠΎΡ ΡΠΈΡΡΠ΅ΠΌΠΈ ΡΡ Π³ΠΎΠ΄ΡΠ²Π»Ρ
The intensity of growth of piglets, their preservation during rearing, and the payment of feed by the increments of animals that were placed for rearing with a design live weight of 7 kg and 20 % less than the design weight β 5.5 kg were studied. Also, the ratio of consumption of compound feed of different recipes during rearing, their cost, and the efficiency of rearing piglets at different staged live weights were studied. It was established that piglets that weighed 1.58 kg less at the beginning of rearing, when placed on rearing during this period, showed 20.9 % lower growth energy, due to which they had 19.6 % lower absolute growth during this period, which caused together with a lower production weight, a 20.3 % lower weight when transferred to fattening and an 8.8 % worse feed payment in increments, they consumed 31.4 % more of the expensive first pre-starter feed during the growing period, and 11.9 % less than the second cheaper pre-starter compound feed and 42.6 % less than the cheapest starter compound feed, as a result of which the cost of feed consumed by the animals of the experimental group was 10.6 % lower compared to the analogs of the experimental group. But taking into account the significantly lower absolute growth of the animals of the experimental group, the cost of feed for 1 kg of growth was 11.2 % higher in comparison with the similar indicator of animals that were put on growing at a designed live weight of 7.0 kg. At the same time, rearing piglets under the conditions of putting them into this process with the design live weight contributed to a decrease of 11.2 % in the cost of feed per kilogram of growth, an increase of 20.3 % in the cost of one piglet after the completion of rearing, and a 23.1 % increase in the income from its sale and 1.07 % higher profitability of raising one head, but resulted in 10.6 % higher feed and operating cost of rearing 1 head and 19.6 % higher operating cost of one piglet at the end of rearing.ΠΠΈΠ²ΡΠ°Π»ΠΈΡΡ ΡΠ½ΡΠ΅Π½ΡΠΈΠ²Π½ΡΡΡΡ ΡΠΎΡΡΡ ΠΏΠΎΡΠΎΡΡΡ, ΡΡ
Π·Π±Π΅ΡΠ΅ΠΆΠ΅Π½ΡΡΡΡ ΠΏΡΠ΄ ΡΠ°Ρ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ ΡΠ° ΠΎΠΏΠ»Π°ΡΠ° ΠΊΠΎΡΠΌΡ ΠΏΡΠΈΡΠΎΡΡΠ°ΠΌΠΈ ΡΠ²Π°ΡΠΈΠ½, ΡΠΊΡ Π±ΡΠ»ΠΈ ΠΏΠΎΡΡΠ°Π²Π»Π΅Π½Ρ Π½Π° Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ Π·Π° ΠΏΡΠΎΠ΅ΠΊΡΠ½ΠΎΡ ΠΆΠΈΠ²ΠΎΡ ΠΌΠ°ΡΠΈ 7 ΠΊΠ³ ΡΠ° Π½Π° 20 % ΠΌΠ΅Π½ΡΠΎΡ Π²ΡΠ΄ ΠΏΡΠΎΠ΅ΠΊΡΠ½ΠΎΡ β 5,5 ΠΊΠ³. Π’Π°ΠΊΠΎΠΆ Π²ΠΈΠ²ΡΠ°Π»ΠΎΡΡ ΡΠΏΡΠ²ΡΠ΄Π½ΠΎΡΠ΅Π½Π½Ρ ΡΠΏΠΎΠΆΠΈΠ²Π°Π½Π½Ρ ΠΊΠΎΠΌΠ±ΡΠΊΠΎΡΠΌΡΠ² ΡΡΠ·Π½ΠΈΡ
ΡΠ΅ΡΠ΅ΠΏΡΡΡ ΠΏΡΠ΄ ΡΠ°Ρ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ, ΡΡ
Π½Ρ Π²Π°ΡΡΡΡΡΡ ΡΠ° Π΅ΡΠ΅ΠΊΡΠΈΠ²Π½ΡΡΡΡ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΏΠΎΡΠΎΡΡΡ Π·Π° ΡΡΠ·Π½ΠΎΡ ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΠΎΡΠ½ΠΎΡ ΠΆΠΈΠ²ΠΎΡ ΠΌΠ°ΡΠΈ. ΠΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Π½ΠΎ, ΡΠΎ ΠΏΠΎΡΠΎΡΡΡΠ°, ΡΠΊΡ ΠΌΠ°Π»ΠΈ Π½Π° ΠΏΠΎΡΠ°ΡΠΎΠΊ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΌΠ΅Π½ΡΡ Π½Π° 1,58 ΠΊΠ³ Π²Π°Π³Ρ, ΠΏΡΠΈ ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΡΡ Π½Π° Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΏΡΠ΄ ΡΠ°Ρ ΡΡΠΎΠ³ΠΎ ΠΏΠ΅ΡΡΠΎΠ΄Ρ Π²ΠΈΡΠ²ΠΈΠ»ΠΈ Π½Π° 20,9 % Π½ΠΈΠΆΡΡ Π΅Π½Π΅ΡΠ³ΡΡ ΡΠΎΡΡΡ, Π·Π° ΡΠ°Ρ
ΡΠ½ΠΎΠΊ ΡΠΎΠ³ΠΎ ΠΌΠ°Π»ΠΈ ΠΌΠ΅Π½ΡΡ Π½Π° 19,6 % Π°Π±ΡΠΎΠ»ΡΡΠ½Ρ ΠΏΡΠΈΡΠΎΡΡΠΈ Π·Π° ΡΠ΅ΠΉ ΠΏΠ΅ΡΡΠΎΠ΄, ΡΠΎ ΡΠΏΡΠΈΡΠΈΠ½ΠΈΠ»ΠΎ ΡΠ°Π·ΠΎΠΌ Π· ΠΌΠ΅Π½ΡΠΎΡ ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΠΎΡΠ½ΠΎΡ ΠΌΠ°ΡΠΎΡ Π½Π° 20,3 % Π½ΠΈΠΆΡΡ ΠΌΠ°ΡΡ ΠΏΡΠΈ ΠΏΠ΅ΡΠ΅Π²Π΅Π΄Π΅Π½Π½Ρ Π½Π° Π²ΡΠ΄Π³ΠΎΠ΄ΡΠ²Π»Ρ ΡΠ° Π³ΡΡΡΡ Π½Π° 8,8 % ΠΎΠΏΠ»Π°ΡΡ ΠΊΠΎΡΠΌΡ ΠΏΡΠΈΡΠΎΡΡΠ°ΠΌΠΈ, Π²ΠΎΠ½ΠΈ ΡΠΏΠΎΠΆΠΈΠ»ΠΈ Π·Π° ΡΠ°Ρ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ Π½Π° 31,4 % Π±ΡΠ»ΡΡΠ΅ Π΄ΠΎΡΠΎΠ³ΠΎΠ³ΠΎ ΠΏΠ΅ΡΡΠΎΠ³ΠΎ ΠΏΡΠ΅ΡΡΠ°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΡΠΌΡ, ΡΠ° Π½Π° 11,9% ΠΌΠ΅Π½ΡΠ΅ Π΄Π΅ΡΠ΅Π²ΡΠΎΠ³ΠΎ Π΄ΡΡΠ³ΠΎΠ³ΠΎ ΠΏΡΠ΅ΡΡΠ°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠ±ΡΠΊΠΎΡΠΌΡ Ρ Π½Π° 42,6% ΠΌΠ΅Π½ΡΠ΅ Π½Π°ΠΉΠ±ΡΠ»ΡΡ Π΄Π΅ ΡΠ΅Π²ΡΠΎΠ³ΠΎ ΡΡΠ°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠΌΠ±ΡΠΊΠΎΡΠΌΡ, Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΎΠ³ΠΎ Π²Π°ΡΡΡΡΡΡ ΡΠΏΠΎΠΆΠΈΡΠΈΡ
ΠΊΠΎΡΠΌΡΠ² ΡΠ²Π°ΡΠΈΠ½Π°ΠΌΠΈ Π΄ΠΎΡΠ»ΡΠ΄Π½ΠΎΡ Π³ΡΡΠΏΠΈ Π²ΠΈΡΠ²ΠΈΠ»ΠΎΡΡ Π½Π° 10,6 % ΠΌΠ΅Π½ΡΠΎΡ ΠΏΠΎΡΡΠ²Π½ΡΠ½ΠΎ Π· Π°Π½Π°Π»ΠΎΠ³Π°ΠΌΠΈ Π΄ΠΎΡΠ»ΡΠ΄Π½ΠΎΡ Π³ΡΡΠΏΠΈ. ΠΠ»Π΅ Π²ΡΠ°Ρ
ΠΎΠ²ΡΡΡΠΈ ΡΡΡΡΡΠ²ΠΎ Π½ΠΈΠΆΡΠΈΠΉ Π°Π±ΡΠΎΠ»ΡΡΠ½ΠΈΠΉ ΠΏΡΠΈΡΡΡΡ Ρ ΡΠ²Π°ΡΠΈΠ½ Π΄ΠΎΡΠ»ΡΠ΄Π½ΠΎΡ Π³ΡΡΠΏΠΈ, ΠΊΠΎΡΠΌΠΎΠ²Π° ΡΠΎΠ±ΡΠ²Π°ΡΡΡΡΡΡ 1 ΠΊΠ³ ΠΏΡΠΈΡΠΎΡΡΡ Ρ Π½ΠΈΡ
Π²ΠΈΡΠ²ΠΈΠ»Π°ΡΡ Π½Π° 11,2 % Π²ΠΈΡΠΎΡ ΠΏΠΎΡΡΠ²Π½ΡΠ½ΠΎ Π· Π°Π½Π°Π»ΠΎΠ³ΡΡΠ½ΠΈΠΌ ΠΏΠΎΠΊΠ°Π·Π½ΠΈΠΊΠΎΠΌ ΡΠ²Π°ΡΠΈΠ½, ΡΠΊΠΈΡ
ΡΡΠ°Π²ΠΈΠ»ΠΈ Π½Π° Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ Π·Π° ΠΏΡΠΎΠ΅ΠΊΡΠ½ΠΎΡ ΠΆΠΈΠ²ΠΎΡ ΠΌΠ°ΡΠΈ 7,0 ΠΊΠ³. ΠΠΎΠ΄Π½ΠΎΡΠ°Ρ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΏΠΎΡΡΡΡ Π·Π° ΡΠΌΠΎΠ² ΠΏΠΎΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ ΡΡ
Π½Π° ΡΠ΅ΠΉ ΠΏΡΠΎΡΠ΅Ρ Π· ΠΏΡΠΎΠ΅ΠΊΡΠ½ΠΎΡ ΠΆΠΈΠ²ΠΎΡ ΠΌΠ°ΡΠΎΡ ΠΏΠΎΡΠΏΡΠΈΡΠ»ΠΎ Π·ΠΌΠ΅Π½ΡΠ΅Π½Π½Ρ Π½Π° 11,2 % ΠΊΠΎΡΠΌΠΎΠ²ΠΎΡ ΡΠΎΠ±ΡΠ²Π°ΡΡΠΎΡΡΡ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΊΡΠ»ΠΎΠ³ΡΠ°ΠΌΠ° ΠΏΡΠΈΡΠΎΡΡΡ, ΠΏΡΠ΄Π²ΠΈΡΠ΅Π½Π½Ρ Π½Π° 20,3 % Π²Π°ΡΡΠΎΡΡΡ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΠΎΡΠΎΡΡΡΠΈ ΠΏΠΎ Π·Π°Π²Π΅ΡΡΠ΅Π½Π½Ρ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ ΡΠ° Π½Π° 23,1 % Π΄ΠΎΡ
ΠΎΠ΄Ρ Π²ΡΠ΄ ΠΉΠΎΠ³ΠΎ ΡΠ΅Π°Π»ΡΠ·Π°ΡΡΡ Ρ Π½Π° 1,07 % Π²ΠΈΡΡΠΉ ΡΠ΅Π½ΡΠ°Π±Π΅Π»ΡΠ½ΠΎΡΡΡ Π²ΠΈΡΠΎΡΡΠ²Π°Π½Π½Ρ ΠΎΠ΄Π½ΡΡΡ Π³ΠΎΠ»ΠΎΠ²ΠΈ, Π°Π»Π΅ ΡΠΏΡΠΈΡΠΈΠ½ΠΈΠ»ΠΎ Π²ΠΈΡΡ Π½Π° 10,6 % ΠΊΠΎΡΠΌΠΎΠ²Ρ ΡΠ° ΠΎΠΏΠ΅ΡΠ°ΡΡΠΉΠ½Ρ ΡΠΎΠ±ΡΠ²Π°ΡΡΡΡΡΡ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ 1 Π³ΠΎΠ»ΠΎΠ²ΠΈ ΡΠ° Π½Π° 19,6 % ΠΎΠΏΠ΅ΡΠ°ΡΡΠΉΠ½Ρ ΡΠΎΠ±ΡΠ²Π°ΡΡΡΡΡΡ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΡΠ΄ΡΠ²ΠΈΠ½ΠΊΠ° Π½Π° ΠΊΡΠ½Π΅ΡΡ Π΄ΠΎΡΠΎΡΡΠ²Π°Π½Π½Ρ
Effectiveness of different systems of liquid feeding of piglets for additional growing in the conditions of industrial technology
The article, a comparative analysis of the productivity of piglets during rearing under a liquid feeding system with fodder mixtures, which were mixed in the feed containers of the Hydro Mix Pro feeding system of the Big Dutchmen company and with the help of the portioned feeding system Spotmix II of the Austrian company Schauer, is made. It was found that the preparation and distribution of feed using the Spotmix II portioned feeding system resulted in 1.5 % better piglet survival, 9.6 % higher piglet growth rate during rearing, 9.5 % higher absolute gains during this period, higher by 7.3 % of the weight of animals when transferred to fattening compared to analogs that were raised on liquid feeding with feed mixing in feed tanks. It has been proven that piglets that were prepared, transported, and distributed feed using the Spotmix II system consumed 6.0 % more feed per day, consumed 7.0 % more during the period, the cost of which was 10.6 % higher. Meanwhile, their feed conversion was 2.3 % better, with almost the exact feed cost per kilogram gain. The feeding of piglets in growing-out using the Spotmix II portioned liquid feeding system led to a 10.6 % higher cost of feed, a 22.1 % higher amortization costs for the equipment for feed distribution and animal feeding, a 9.6 % higher cost of the growing-out process of one pig, and its cost price at the end of the growing period is 3.4 times higher. At the same time, such feeding contributed to higher growth energy of animals during rearing, which caused a 7.3 % higher sales price of piglets, a 17.3 % higher profit from the sale of one head, and a 5.2 % higher profitability of rearing piglets compared to liquid feeding using Hydro Mix Pro system with feed mixing in feed tanks
Measurement of Muon Capture on the Proton to 1% Precision and Determination of the Pseudoscalar Coupling g_P
The MuCap experiment at the Paul Scherrer Institute has measured the rate L_S
of muon capture from the singlet state of the muonic hydrogen atom to a
precision of 1%. A muon beam was stopped in a time projection chamber filled
with 10-bar, ultra-pure hydrogen gas. Cylindrical wire chambers and a segmented
scintillator barrel detected electrons from muon decay. L_S is determined from
the difference between the mu- disappearance rate in hydrogen and the free muon
decay rate. The result is based on the analysis of 1.2 10^10 mu- decays, from
which we extract the capture rate L_S = (714.9 +- 5.4(stat) +- 5.1(syst)) s^-1
and derive the proton's pseudoscalar coupling g_P(q^2_0 = -0.88 m^2_mu) = 8.06
+- 0.55.Comment: Updated figure 1 and small changes in wording to match published
versio
Measurement of the Rate of Muon Capture in Hydrogen Gas and Determination of the Proton's Pseudoscalar Coupling
The rate of nuclear muon capture by the proton has been measured using a new
experimental technique based on a time projection chamber operating in
ultra-clean, deuterium-depleted hydrogen gas at 1 MPa pressure. The capture
rate was obtained from the difference between the measured
disappearance rate in hydrogen and the world average for the decay
rate. The target's low gas density of 1% compared to liquid hydrogen is key to
avoiding uncertainties that arise from the formation of muonic molecules. The
capture rate from the hyperfine singlet ground state of the atom is
measured to be , from which the induced
pseudoscalar coupling of the nucleon, , is
extracted. This result is consistent with theoretical predictions for
that are based on the approximate chiral symmetry of QCD.Comment: submitted to Phys.Rev.Let
Isolation, crystallization, and investigation of ribosomal protein S8 complexed with specific fragments of rRNA of bacterial or archaeal origin. Biochemistry 66
Study of the nature of protein-rRNA complexes is a topical problem of modern molecular biology. Structural studies of rRNA-protein complexes are the most direct and precise method of analysis of these interactions. Because ribosomal proteins are most conservative during evolution, their complexes with specific RNA fragments provide an interesting model for studying RNA-protein interactions. Ribosomal protein S8 from E. coli plays a key role in assembling the small ribosomal subunit The major region of protein S8 binding on 16S rRNA was determined by partial hydrolysis with restric tion endonucleases The binding sites of protein S8 on 16S rRNA are similar in E. coli and T. thermophilus. It was shown that ACCELERATED PUBLICATION 0006 2979/01/6609 0948$25.00 Β©2001 MAIK "Nauka / Interperiodica" * To whom correspondence should be addressed. Vol. 66, No. 9, 2001, pp. 948 953. Translated from Biokhimiya, Vol. 66, No. 9, 2001, pp. 1165 1171. Original Russian Text Copyright Β© 2001 Abstract-The core ribosomal protein S8 binds to the central domain of 16S rRNA independently of other ribosomal proteins and is required for assembling the 30S subunit. It has been shown with E. coli ribosomes that a short rRNA fragment restrict ed by nucleotides 588 602 and 636 651 is sufficient for strong and specific protein S8 binding. In this work, we studied the complexes formed by ribosomal protein S8 from Thermus thermophilus and Methanococcus jannaschii with short rRNA frag ments isolated from the same organisms. The dissociation constants of the complexes of protein S8 with rRNA fragments were determined. Based on the results of binding experiments, rRNA fragments of different length were designed and syn thesized in preparative amounts in vitro using T7 RNA polymerase. Stable S8-RNA complexes were crystallized. Crystals were obtained both for homologous bacterial and archaeal complexes and for hybrid complexes of archaeal protein with bac terial rRNA. Crystals of the complex of protein S8 from M. jannaschii with the 37 nucleotide rRNA fragment from the same organism suitable for X ray analysis were obtained
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