1,034 research outputs found
Productivity of corn hybrids in relation to the seeding rate
ArticlePotential yield of corn hybrids with a different FAO number is limited by not only
rainfall amount, average soil and air temperature throughout vegetation period, but also directly
depends on plant density. The study and practical application of special agricultural techniques
allows us to limit and mitigate the negative impact of these factors on the productivity of maize,
depending on the indicators under study and the soil and climatic resources of the cultivation
zone. Therefore, the study of the influence of the seeding rate on the growth and development of
corn plants remains relevant. The results presented make it possible to choose optimal seeding
rates for corn hybrids of early and middle groups of ripeness (FAO 180-280). Overcrowding from
61,000 to 93,000 seeds ha-1
leads to increase in interstage period 'sproutingβwax ripeness' of
Rodnik 179SV hybrid for 4 days, of MAS 12R and AMELIOR hybridsβfor 2 days, and of MAS
30K hybrid β for 3 days. Hybrids Rodnik 179SV and AMELIOR reached maximum height β
217 cm and 214 cm respectively β at seeding rate of 73,000 seeds ha-1
, while hybrids MAS 12R and
MAS 30K grew up to their 213 cm and 223 cm respectively at seeding rate of 77,000 seeds ha-1
.
Decrease in seeding rate to less than 73,000 seeds ha-1
and, contrary to it, overcrowding of seeds of
more than 77,000 seeds ha-1
leads to decrease in corn hybrid plant height. Agronomically, the most
efficient for maximizing early ripe Rodnik 179SV and MAS 12R hybrids yields (6.39 and
6.73 t ha-1
) and middle-early ripe AMELIOR hybrid yield (6.81 t ha-1
) was the seeding rate of
73,000 seeds ha-1
, while the highest yield of middle MAS 30K hybrid (7.21 t ha-1
) was at the
seeding rate of 77,000 seeds ha-1
Canted antiferromagnetic phase of the quantum Hall state in bilayer graphene
Motivated to understand the nature of the strongly insulating quantum
Hall state in bilayer graphene, we develop the theory of the state in the
framework of quantum Hall ferromagnetism. The generic phase diagram, obtained
in the presence of the isospin anisotropy, perpendicular electric field, and
Zeeman effect, consists of the spin-polarized ferromagnetic (F), canted
antiferromagnetic (CAF), and partially (PLP) and fully (FLP) layer-polarized
phases. We address the edge transport properties of the phases. Comparing our
findings with the recent data on suspended dual-gated devices, we conclude that
the insulating state realized in bilayer graphene at lower electric
field is the CAF phase. We also predict a continuous and a sharp
insulator-metal phase transition upon tilting the magnetic field from the
insulating CAF and FLP phases, respectively, to the F phase with metallic edge
conductance , which could be within the reach of available fields and
could allow one to identify and distinguish the phases experimentally.Comment: 5 pages, 3 figs; v2: published versio
Plasmonic nanostructures with local temporal response: a platform for time-varying photonics
This work is devoted to the development of an approach for implementation and designing time-varying media. A mechanism based on the use of plasmonic nanostructures with a reduced plasmon lifetime is proposed. It is shown that such nanostructures can be used to enhance the strength and speed of modulation of the refractive index ofnonlinear media. This is achieved through decreasing of the spectral dispersion of the real permittivity. Plasmonic materials with peculiar optical properties, such as flatdispersion in the near-infrared range, were synthesized. For this purpose, we prepared TiON thin films and performed thermal post-treatment for fine-tuning permittivity of TiON. It has been shown that the proposed materials allow one to achieve an ultrashort plasmon lifetime on the order of 0.1 fs, which is an order of magnitude shorter than in the case of traditional plasmonic materials
Subexponential estimations in Shirshov's height theorem (in English)
In 1993 E. I. Zelmanov asked the following question in Dniester Notebook:
"Suppose that F_{2, m} is a 2-generated associative ring with the identity
x^m=0. Is it true, that the nilpotency degree of F_{2, m} has exponential
growth?" We show that the nilpotency degree of l-generated associative algebra
with the identity x^d=0 is smaller than Psi(d,d,l), where Psi(n,d,l)=2^{18} l
(nd)^{3 log_3 (nd)+13}d^2. We give the definitive answer to E. I. Zelmanov by
this result. It is the consequence of one fact, which is based on combinatorics
of words. Let l, n and d>n be positive integers. Then all the words over
alphabet of cardinality l which length is greater than Psi(n,d,l) are either
n-divided or contain d-th power of subword, where a word W is n-divided, if it
can be represented in the following form W=W_0 W_1...W_n such that W_1 >'
W_2>'...>'W_n. The symbol >' means lexicographical order here. A. I. Shirshov
proved that the set of non n-divided words over alphabet of cardinality l has
bounded height h over the set Y consisting of all the words of degree <n.
Original Shirshov's estimation was just recursive, in 1982 double exponent was
obtained by A.G.Kolotov and in 1993 A.Ya.Belov obtained exponential estimation.
We show, that h<Phi(n,l), where Phi(n,l) = 2^{87} n^{12 log_3 n + 48} l. Our
proof uses Latyshev idea of Dilworth theorem application.Comment: 21 pages, Russian version of the article is located at the link
arXiv:1101.4909; Sbornik: Mathematics, 203:4 (2012), 534 -- 55
Strong focusing higher-order laser modes: Transverse and longitudinal optical fields
Β© Published under licence by IOP Publishing Ltd. The distribution of transverse and longitudinal optical fields in tightly focused higher-order laser beams is investigated. Polarization-dependent fingerprints of transverse and longitudinal optical fields are experimentally captured by means of photoinduced surface deformations in azobenzene polymer thin films
Π¦ΠΠΠΠΠΠΠΠΠΠ Π’ΠΠ Π‘ ΠΠΠΠΠΠΠΠ ΠΠΠΠΠΠ«Π ΠΠΠΠΠΠΠ Π£ΠΠ ΠΠΠΠΠΠΠ― ΠΠΠ― Π‘ΠΠ‘Π’ΠΠ ΠΠΠΠΠ’Π ΠΠ‘ΠΠΠΠΠΠΠΠ― ΠΠΠ’ΠΠΠΠΠΠ«Π₯ ΠΠΠͺΠΠΠ’ΠΠ
The present paper considers cycle-converter with complicated control law. The methodj complicated control law generating is presented. The scheme of power circuits is introduced. VoltaΒ and current curves for classical cycle-converter and cycle-converter with complicated control lawiΒ discussed. Introducing of complicated control law improves output voltage quality, increaΒ fundamental harmonic's amplitude and input power factor. The article is attractive in the field of iΒ power electronics.Π ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ ΡΠΈΠΊΠ»ΠΎΠΊΠΎΠ½Π²Π΅ΡΡΠ΅Ρ Ρ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ Π·Π°ΠΊΠΎΠ½ΠΎΠΌ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡΒ Π²Π΅Π½ΡΠΈΠ»ΡΠ½ΡΠΌΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ°ΠΌΠΈ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ ΡΠΏΠΎΡΠΎΠ± ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°Β ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΡΡ
Π΅ΠΌΠ° ΡΠΈΠ»ΠΎΠ²ΡΡ
ΡΠ΅ΠΏΠ΅ΠΉ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ. Π Π°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΡΡΒ ΡΠΏΡΡΡ ΠΊΡΠΈΠ²ΡΡ
Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΈ ΡΠΎΠΊΠ° Π΄Π»Ρ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡ
Π΅ΠΌΡ ΡΠΈΠΊΠ»ΠΎΠΊΠΎΠ½Π²Π΅ΡΡΠ΅ΡΠ° ΠΈ Π΄Π»ΡΒ ΡΡ
Π΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ Ρ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ Π·Π°ΠΊΠΎΠ½ΠΎΠΌ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ. ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎΒ ΡΠΈΠ³Π½Π°Π»Π° ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΏΠΎΠ²ΡΡΠ°Π΅Ρ ΠΊΠ°ΡΠ΅ΡΡΠ²ΠΎ Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ, ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π΅Ρ Π°ΠΌΠΏΠ»ΠΈΡΡΠ΄ΡΒ ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΉ Π³Π°ΡΠΌΠΎΠ½ΠΈΠΊΠΈ ΠΈ Π²Ρ
ΠΎΠ΄Π½ΠΎΠΉ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½Ρ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ. Π‘ΡΠ°ΡΡΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΠΈΠ½ΡΠ΅ΡΠ΅Ρ Π΄Π»ΡΒ ΡΠΏΠ΅ΡΠΈΠ°Π»ΠΈΡΡΠΎΠ² Π² ΠΎΠ±Π»Π°ΡΡΠΈ Π°Π²ΠΈΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΈΠ»ΠΎΠ²ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠΈ.Π ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ ΡΠΈΠΊΠ»ΠΎΠΊΠΎΠ½Π²Π΅ΡΡΠ΅Ρ Ρ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ Π·Π°ΠΊΠΎΠ½ΠΎΠΌ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡΒ Π²Π΅Π½ΡΠΈΠ»ΡΠ½ΡΠΌΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ°ΠΌΠΈ. ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ ΡΠΏΠΎΡΠΎΠ± ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°Β ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Π° ΡΡ
Π΅ΠΌΠ° ΡΠΈΠ»ΠΎΠ²ΡΡ
ΡΠ΅ΠΏΠ΅ΠΉ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠ³ΠΎ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ. Π Π°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°ΡΡΡΡΒ ΡΠΏΡΡΡ ΠΊΡΠΈΠ²ΡΡ
Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ ΠΈ ΡΠΎΠΊΠ° Π΄Π»Ρ ΠΊΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡ
Π΅ΠΌΡ ΡΠΈΠΊΠ»ΠΎΠΊΠΎΠ½Π²Π΅ΡΡΠ΅ΡΠ° ΠΈ Π΄Π»ΡΒ ΡΡ
Π΅ΠΌΡ ΠΏΡΠ΅ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°ΡΠ΅Π»Ρ Ρ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ Π·Π°ΠΊΠΎΠ½ΠΎΠΌ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ. ΠΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎΒ ΡΠΈΠ³Π½Π°Π»Π° ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΏΠΎΠ²ΡΡΠ°Π΅Ρ ΠΊΠ°ΡΠ΅ΡΡΠ²ΠΎ Π²ΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ, ΡΠ²Π΅Π»ΠΈΡΠΈΠ²Π°Π΅Ρ Π°ΠΌΠΏΠ»ΠΈΡΡΠ΄ΡΒ ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠΉ Π³Π°ΡΠΌΠΎΠ½ΠΈΠΊΠΈ ΠΈ Π²Ρ
ΠΎΠ΄Π½ΠΎΠΉ ΠΊΠΎΡΡΡΠΈΡΠΈΠ΅Π½Ρ ΠΌΠΎΡΠ½ΠΎΡΡΠΈ. Π‘ΡΠ°ΡΡΡ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅Ρ ΠΈΠ½ΡΠ΅ΡΠ΅Ρ Π΄Π»ΡΒ ΡΠΏΠ΅ΡΠΈΠ°Π»ΠΈΡΡΠΎΠ² Π² ΠΎΠ±Π»Π°ΡΡΠΈ Π°Π²ΠΈΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠΈΠ»ΠΎΠ²ΠΎΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠΈ
ΠΠ΅ΠΎΠ΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠ°Ρ ΠΌΠΎΠ΄Π΅Π»Ρ Π³Π»ΡΠ±ΠΈΠ½Π½ΠΎΠ³ΠΎ ΡΡΡΠΎΠ΅Π½ΠΈΡ ΠΏΠ°Π»Π΅ΠΎΡΡΠ±Π΄ΡΠΊΡΠΈΠΎΠ½Π½ΠΎΠΉ Π·ΠΎΠ½Ρ Π½Π° Π²ΠΎΡΡΠΎΡΠ½ΠΎΠΉ ΠΎΠΊΡΠ°ΠΈΠ½Π΅ Π ΡΡΡΠΊΠΎΠΉ ΠΏΠ°Π»Π΅ΠΎΠΏΠ»ΠΈΡΡ ΠΈ ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΌΠ΅ΡΡΠΎΡΠΎΠΆΠ΄Π΅Π½ΠΈΠΉ Π½Π΅ΡΡΠΈ ΠΈ Π³Π°Π·Π°
Known hypothesis of M. Barazangi that quasilinear geological and tectonic zones represent the banded structures, which are parallel to the Urals paleo volcanic mountain belt was used. These zones can be in some interval of distances from a mountain paleo volcanic belt. On the size of this interval (~ 103 km) and the periodical arrangement of quasilinear geological and tectonic zones (of about ~ 300 km width), the paleo subduction speed (~ 5 β 6 cm a year) was estimated on the example of some Siberian regions.ΠΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Π° ΠΈΠ·Π²Π΅ΡΡΠ½Π°Ρ Π³ΠΈΠΏΠΎΡΠ΅Π·Π° M. Barazangi ΠΎ ΡΠΎΠΌ, ΡΡΠΎ ΠΊΠ²Π°Π·ΠΈΠ»ΠΈΠ½Π΅ΠΉΠ½ΡΠ΅ Π³Π΅ΠΎΠ»ΠΎΠ³ΠΎ-ΡΠ΅ΠΊΡΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π·ΠΎΠ½Ρ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΡΡ ΡΠΎΠ±ΠΎΠΉ ΠΏΠΎΠ»ΠΎΡΡΠ°ΡΡΠ΅ ΡΡΡΡΠΊΡΡΡΡ, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΏΠ°ΡΠ°Π»Π»Π΅Π»ΡΠ½Ρ ΠΏΠ°Π»Π΅ΠΎΠ²ΡΠ»ΠΊΠ°Π½ΠΈΡΠ΅ΡΠΊΠΎΠΌΡ Π£ΡΠ°Π»ΡΡΠΊΠΎΠΌΡ Π³ΠΎΡΠ½ΠΎΠΌΡ ΠΏΠΎΡΡΡ ΠΈ ΠΌΠΎΠ³ΡΡ Π½Π°Ρ
ΠΎΠ΄ΠΈΡΡΡΡ Π² ΠΏΡΠ΅Π΄Π΅Π»Π°Ρ
Π½Π΅ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π° ΡΠ°ΡΡΡΠΎΡΠ½ΠΈΠΉ ΠΎΡ ΠΏΠΎΡΡΠ°. ΠΠΎ Π²Π΅Π»ΠΈΡΠΈΠ½Π΅ ΡΡΠΎΠ³ΠΎ ΠΈΠ½ΡΠ΅ΡΠ²Π°Π»Π° (~10 3 ΠΊΠΌ) ΠΈ ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠΌΡ ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΡ ΠΊΠ²Π°Π·ΠΈΠ»ΠΈΠ½Π΅ΠΉΠ½ΡΡ
Π³Π΅ΠΎΠ»ΠΎΠ³ΠΎ-ΡΠ΅ΠΊΡΠΎΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
Π·ΠΎΠ½ (Ρ ΠΏΠΎΠΏΠ΅ΡΠ΅ΡΠ½ΡΠΌ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠΌ ~ 300 ΠΊΠΌ) ΠΎΡΠ΅Π½ΠΈΠ²Π°Π΅ΡΡΡ ΡΠΊΠΎΡΠΎΡΡΡ ΠΏΠ°Π»Π΅ΠΎΡΡΠ±Π΄ΡΠΊΡΠΈΠΈ (~ 5 β 6 ΡΠΌ Π² Π³ΠΎΠ΄) Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ Π½Π΅ΠΊΠΎΡΠΎΡΡΡ
ΡΠ°ΠΉΠΎΠ½ΠΎΠ² Π‘ΠΈΠ±ΠΈΡΠΈ. ΠΠ»ΡΡΠ΅ΡΠ½Π°ΡΠΈΠ²ΠΎΠΉ ΡΡΠΎΠ»Ρ Π²ΡΡΠΎΠΊΠΎΠΉ ΡΠΊΠΎΡΠΎΡΡΠΈ ΠΏΠ°Π»Π΅ΠΎΡΡΠ±Π΄ΡΠΊΡΠΈΠΈ ΠΌΠΎΠΆΠ΅Ρ Π±ΡΡΡ ΡΠ³ΠΎΠ» ΠΏΠ°Π»Π΅ΠΎΡΡΠ±Π΄ΡΠΊΡΠΈΠΈ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ ΠΌΠ΅Π½ΡΡΠ΅ 10Β°. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠ°ΡΡΠ΅ΡΠ° ΠΌΠΎΠ³ΡΡ Π±ΡΡΡ ΠΏΡΠΈΠΌΠ΅Π½ΠΈΠΌΡ ΠΏΡΠΈ ΠΈΠ·ΡΡΠ΅Π½ΠΈΠΈ Π΄ΡΠ΅Π²Π½ΠΈΡ
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