177 research outputs found

    ЀСртигация Ρ‚ΠΎΠΌΠ°Ρ‚Π° Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ Π³Ρ€ΡƒΠ½Ρ‚Π΅

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    Obtaining high and stable yields of tomato with good consumer qualities in the open field has now become problematic due to the fact that hybrids and varieties of tomato of an intensive type place high demands on the presence of moisture and nutrients in the root-soil layer. The required level of soil moisture in combination with the introduction of calculated doses of mineral fertilizers during the growing season provides for obtaining the planned yields of vegetables, including tomato. The most important resource for the further development of agriculture in the Russian Federation is irrigated land. Volgograd region is one of the largest irrigated agricultural regions in Russia. Growing of almost all vegetables in the region is conducted on irrigated lands. The use of only one irrigation without the use of fertilizers will not have a positive impact on the growth, development and productivity of plants. Fertigation is the most effective and economical way of delivering nutrients to the plant root system and allows to get a higher yields than other methods of fertilizer application. In fertigation systems, the control of optimal concentrations of fertilizers is easily achieved, their ratio and these parameters can be controlled automatically. The purpose of this work was to study the comparative efficiency of ammonium nitrate, calcium nitrate and a combination of calcium nitrate and ammonium chloride for tomato fertigation in combination with non-root dressings of complex water-soluble fertilizers containing macroand microelements in open feild on irrigated lighchestnut soil of dry steppe zone of chestnut soils in the Volgograd region. As a result, analysis of the use of mineral fertilizers for tomato fertigation in light chestnut soils of the Volgograd region was carried out. The positive effect of foliar dressing with microelements in the proposed dosages has been proven.Π‘ΠΎΠ²Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹Π΅ сорта ΠΈ Π³ΠΈΠ±Ρ€ΠΈΠ΄Ρ‹ Π²ΠΎΠ·Π΄Π΅Π»Ρ‹Π²Π°Π΅ΠΌΡ‹Π΅ Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ Π³Ρ€ΡƒΠ½Ρ‚Π΅ ΠΎΡ‡Π΅Π½ΡŒ Ρ‚Ρ€Π΅Π±ΠΎΠ²Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹ ΠΊ Π½Π°Π»ΠΈΡ‡ΠΈΡŽ Π²Π»Π°Π³ΠΈ ΠΈ ΠΏΠΈΡ‚Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… вСщСств Π² ΠΏΠΎΡ‡Π²Π΅. ИсслСдовано ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Ρ„Π΅Ρ€Π³Π΅Ρ‚Π°Ρ†ΠΈΠΈ для ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½ΠΈΡ устойчивости Ρ‚ΠΎΠΌΠ°Ρ‚ΠΎΠ² Π½Π° ΠΎΡ€ΠΎΡˆΠ°Π΅ΠΌΡ‹Ρ… зСмлях. Π˜Π·ΡƒΡ‡Π΅Π½Π° ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Π°Ρ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ использования Π°ΠΌΠΌΠΈΠ°Ρ‡Π½ΠΎΠΉ сСлитры, ΠΊΠ°Π»ΡŒΡ†ΠΈΠ΅Π²ΠΎΠΉ сСлитры (Π½ΠΈΡ‚Ρ€Π°Ρ‚Π° ΠΊΠ°Π»ΡŒΡ†ΠΈΡ) ΠΈ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ ΠΊΠ°Π»ΡŒΡ†ΠΈΠ΅Π²ΠΎΠΉ сСлитры ΠΈ Ρ…Π»ΠΎΡ€ΠΈΠ΄Π° аммония для Ρ„Π΅Ρ€Ρ‚ΠΈΠ³Π°Ρ†ΠΈΠΈ Ρ‚ΠΎΠΌΠ°Ρ‚Π° Π² сочСтании с Π½Π΅ΠΊΠΎΡ€Π½Π΅Π²Ρ‹ΠΌΠΈ ΠΏΠΎΠ΄ΠΊΠΎΡ€ΠΌΠΊΠ°ΠΌΠΈ комплСксными водорастворимыми удобрСниями, содСрТащими ΠΌΠ°ΠΊΡ€ΠΎΠΈ микроэлСмСнты, Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ Π³Ρ€ΡƒΠ½Ρ‚Π΅ Π½Π° ΠΎΡ€ΠΎΡˆΠ°Π΅ΠΌΠΎΠΉ свСтло-ΠΊΠ°ΡˆΡ‚Π°Π½ΠΎΠ²ΠΎΠΉ ΠΏΠΎΡ‡Π²Π΅ сухостСпной Π·ΠΎΠ½Ρ‹ ΠΊΠ°ΡˆΡ‚Π°Π½ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΡ‡Π² Волгоградской области. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ Π°Π½Π°Π»ΠΈΠ· использования ΠΌΠΈΠ½Π΅Ρ€Π°Π»ΡŒΠ½Ρ‹Ρ… ΡƒΠ΄ΠΎΠ±Ρ€Π΅Π½ΠΈΠΉ для Ρ„Π΅Ρ€Ρ‚ΠΈΠ³Π°Ρ†ΠΈΠΈ Ρ‚ΠΎΠΌΠ°Ρ‚Π° Π² условиях свСтло-ΠΊΠ°ΡˆΡ‚Π°Π½ΠΎΠ²Ρ‹Ρ… ΠΏΠΎΡ‡Π² Волгоградской области. Π”ΠΎΠΊΠ°Π·Π°Π½ΠΎ ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ΅ влияниС листовых ΠΏΠΎΠ΄ΠΊΠΎΡ€ΠΌΠΎΠΊ микроэлСмСнтами Π² ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½Ρ‹Ρ… Π΄ΠΎΠ·ΠΈΡ€ΠΎΠ²ΠΊΠ°Ρ…

    Search for direct production of a2(1320) and f2(1270) mesons in e+e- annihilation

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    A search for direct production of C-even resonances a2(1320) and f2(1270) in e+e- annihilation was performed with SND detector at VEPP-2M e+e- collider. The upper limits of electronic widths of these mesons were obtained at 90% confidence level: Gamma(a2(1320) \to e+e-) < 0.56 eV, Gamma(f2(1270) \to e+e-) < 0.11 eV.Comment: 6 pages, 5 figures, 1 table. Submitted to Phys. Lett.

    The process e+eβˆ’β†’Ο€+Ο€βˆ’Ο€0e^+e^-\to\pi^+\pi^-\pi^0 in the energy range 2E_0=1.04 - 1.38 GeV

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    In the experiment with the SND detector at VEPP-2M e^+e^- collider the process e+eβˆ’β†’Ο€+Ο€βˆ’Ο€0e^+e^-\to\pi^+\pi^-\pi^0 was studied in the energy range 2E_0 from 1.04 to 1.38 GeV. A broad peak was observed with the visible mass Mvis=1220Β±20M_{vis}=1220\pm 20 MeV and cross section in the maximum Οƒ0≃4\sigma_0\simeq 4 nb. The peak can be interpreted as a Ο‰\omega-like resonance Ο‰(1200)\omega (1200).Comment: 10 pages LATEX and 5 figure

    Experimental Study of rho -> pi0 pi0 gamma and omega -> pi0 pi0 gamma Decays

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    The e+e- -> pi0 pi0 gamma process was studied in the SND experiment at VEPP-2M e+e- collider in the energy region 0.60-0.97 GeV. From the analysis of the energy dependence of measured cross section the branching ratios B(omega -> pi0 pi0 gamma)= (6.6 +1.4-0.8(stat) +-0.6(syst))x10^-5 and B(rho -> pi0 pi0 gamma)=(4.1 +1.0-0.9(stat) +-0.3(syst))x10^-5 were obtained.Comment: 16 pages, 7 figures, submitted to Phys. Lett.

    New Data from SND Detector in Novosibirsk

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    The current status of experiments with SND detector at VEPP-2M e^+e^- collider in the energy range 2E_0=400-1400 MeV and recent results of data analysis for Ο•\phi, Ο‰\omega and ρ\rho decays and e^+e^- annihilation into hadrons are presented.Comment: 7 pages, 8 figures, Latex2e, uses espcrc1.sty. Talk given at 8th International Conference on Hadron Spectroscopy (HADRON 99), Beijing, China, 24-28 Aug 199

    Experimental study of the e+e- -> pi0 gamma process in the energy region sqrt(s)=0.60-0.97 GeV

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    Results of the study of the e+e-->pi0 gamma process with SND detector at VEPP-2M collider in the c.m.s. energy range sqrt(s)=0.60-0.97 GeV are presented. Using 36513 selected events corresponding to a total integrated luminosity of 3.4 pb^-1 the e+e-->pi0 gamma cross section was measured. The energy dependence of the cross section was analyzed in the framework of the vector meson dominance model. The data are well described by a sum of phi,omega,rho0->pi0 gamma decay contributions with measured decay probabilities: Br(omega->pi0 gamma)=(9.34+-0.15+-0.31)% and Br(rho0->pi0 gamma)=(5.15+-1.16+-0.73)*10^-4 . The rho-omega relative interference phase is phi(rho,omega}=(-10.2+-6.5+-2.5) degree

    New precise determination of the \tau lepton mass at KEDR detector

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    The status of the experiment on the precise Ο„\tau lepton mass measurement running at the VEPP-4M collider with the KEDR detector is reported. The mass value is evaluated from the Ο„+Ο„βˆ’\tau^+\tau^- cross section behaviour around the production threshold. The preliminary result based on 6.7 pbβˆ’1^{-1} of data is mΟ„=1776.80βˆ’0.23+0.25Β±0.15m_{\tau}=1776.80^{+0.25}_{-0.23} \pm 0.15 MeV. Using 0.8 pbβˆ’1^{-1} of data collected at the Οˆβ€²\psi' peak the preliminary result is also obtained: Ξ“eeBττ(Οˆβ€²)=7.2Β±2.1\Gamma_{ee}B_{\tau\tau}(\psi') = 7.2 \pm 2.1 eV.Comment: 6 pages, 8 figures; The 9th International Workshop on Tau-Lepton Physics, Tau0

    Study of the radiative decay Ο•β†’Ξ·Ξ³\phi \to \eta \gamma with CMD-2 detector

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    Using the 1.9pbβˆ’11.9 pb^{-1} of data collected with the CMD-2 detector at VEPP-2M the decay mode Ο•β†’Ξ·Ξ³\phi \to \eta \gamma, Ξ·β†’Ο€+Ο€βˆ’Ο€0\eta \to \pi^+\pi^-\pi^0 has been studied. The obtained branching ratio is B(Ο•β†’Ξ·Ξ³)=(1.18Β±0.03Β±0.06)\phi \to \eta \gamma) = (1.18 \pm 0.03 \pm 0.06) %.Comment: 13 pages, 5 figures, LaTex2e, to be published in Phys. Lett.

    Observation of KS0K_S^0 semileptonic decays with CMD-2 detector

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    The decay KS0β†’Ο€eΞ½K_S^0 \to \pi e \nu has been observed by the CMD-2 detector at the e^+e^- collider VEPP-2M at Novosibirsk. Of 6 million produced KL0KS0K_L^0K_S^0 pairs, 75Β±1375 \pm 13 events of the KS0β†’Ο€eΞ½K_S^0 \to \pi e \nu decay were selected. The corresponding branching ratio is B(KS0β†’Ο€eΞ½)=(7.2Β±1.4)Γ—10βˆ’4B(K_S^0 \to \pi e \nu)=(7.2 \pm 1.4)\times10^{-4}. This result is consistent with the evaluation of B(KS0β†’Ο€eΞ½)B(K_S^0 \to \pi e \nu) from the KL0K_L^0 semileptonic rate and KS0K_S^0 lifetime assuming Ξ”S=Ξ”Q\Delta S=\Delta Q .Comment: 7 pages, 6 figures, LaTex2e. Submitted to Phys.Lett.

    Measurement of omega meson parameters in pi^+pi^-pi^0 decay mode with CMD-2

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    About 11 200 e^+e^- -> omega -> pi^+pi^-pi^0 events selected in the center of mass energy range from 760 to 810 MeV were used for the measurement of the \omega meson parameters. The following results have been obtained: sigma _{0}=(1457 \pm 23 \pm 19)nb, m_{\omega}=(782.71 \pm 0.07 \pm 0.04) MeV/c^{2}, \Gamma_{\omega}=(8.68 \pm 0.23 \pm 0.10) MeV, \Gamma_{e^+e^-}\cdot Br (\omega -> pi^+pi^-pi^0)= (0.528 \pm 0.012 \pm 0.007) \cdot 10^{-3} MeV.Comment: 8 pages, 4 figure
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