443 research outputs found

    Influence of State Banks on Economic Growth: A Cross-Country Analysis

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    The authors systematize the economic-mathematical models, as well as the results of empirical studies of authoritative international analytical agencies and financial institutions, in which the influence of state capital in the banking system on the development of national economies was formalized on different countries in different periods. The analysis showed that such studies often give some completely opposite results. The reason for these authors is that the sample of countries in these models is formed mainly taking into account differences in the scale of state participation and levels of economic development of countries. This approach is erroneous because it does not take into account the specifics of the construction of the financial sector in these countries and the functions performed by the state banks

    Influence of fluorination time on surface flashover of epoxy in insulating gas

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    The accumulation of charges on polymeric insulation under high voltage DC stress is a major concern in the transmission system as its formation distorts the local electric field and has an adverse impact on the electrical performance. By undergoing fluorination treatment on the insulation, improved surface properties similar to fluoropolymers can be attained without changing the bulk properties of the original material. The change in chemical components at the surface of polymeric insulation should lead to a corresponding change in electrical properties at the surface and thus can suppress charge build up. Previous research on surface flashover on fluorinated epoxy resin at atmospheric condition shows a significant improvement in flashover strength. In this paper, the authors investigated the effect of different degree of fluorination treatment on cast epoxy resin on suppressing surface charge accumulation and its contribution towards the improvement in surface breakdown strength. In comparison to previous research, it has been found that there is an optimum time duration of fluorination treatment which improves the surface breakdown strength of epoxy spacer. The mechanisms that govern the effect of fluorination treatment on surface flashover were discussed

    Mechanical Properties of Friction Stir-Welded Joints of Aluminum Alloys

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    Mechanical properties, intergranular corrosion, and a chemical composition of the welded joint, produced with friction stir welding of a 6061T651 aluminum alloy were investigated. The results show that the welded seam is uniform, with a smooth surface. There are no deformation and defects, such as cracks or gas-filled porosity. The average tensile strength of welded joints is 73% of that of the base material, while the average yield strength and elongation are only 54% and 43% of those of the base material. After intergranular corrosion, microhardness changes evidently and corrosion resistance is lower in the root of the weld nugget zone. The change in microhardness is not pronounced in the weld nugget zone and welded surface, but the change in microhardness is well-pronounced and corrosion resistance is lower in the thermomechanically- and heat-affected zones.Π˜ΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Ρ‹ мСханичСскиС свойства, мСТкристаллитная коррозия ΠΈ химичСский состав сварного шва, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½ΠΎΠ³ΠΎ Ρ€ΠΎΡ‚Π°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ сваркой Ρ‚Ρ€Π΅Π½ΠΈΠ΅ΠΌ, алюминиСвого сплава 6061Π’651. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠΊΠ°Π·Ρ‹Π²Π°ΡŽΡ‚, Ρ‡Ρ‚ΠΎ сварной шов Ρ€Π°Π²Π½ΠΎΠΌΠ΅Ρ€Π΅Π½, ΠΈΠΌΠ΅Π΅Ρ‚ Π³Π»Π°Π΄ΠΊΡƒΡŽ ΠΏΠΎΠ²Π΅Ρ€Ρ…Π½ΠΎΡΡ‚ΡŒ. ΠžΡ‚ΡΡƒΡ‚ΡΡ‚Π²ΡƒΡŽΡ‚ дСформация ΠΈ Ρ‚Π°ΠΊΠΈΠ΅ Π΄Π΅Ρ„Π΅ΠΊΡ‚Ρ‹, ΠΊΠ°ΠΊ Ρ‚Ρ€Π΅Ρ‰ΠΈΠ½Ρ‹ ΠΈΠ»ΠΈ газонасыщСнная ΠΏΠΎΡ€ΠΈΡΡ‚ΠΎΡΡ‚ΡŒ. Π‘Ρ€Π΅Π΄Π½ΠΈΠΉ ΠΏΡ€Π΅Π΄Π΅Π» прочности ΠΏΡ€ΠΈ растяТСнии для сварных соСдинСний составляСт 73% Ρ‚Π°ΠΊΠΎΠ²ΠΎΠ³ΠΎ для основного ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°, Ρ‚ΠΎΠ³Π΄Π° ΠΊΠ°ΠΊ ΠΏΡ€Π΅Π΄Π΅Π» тСкучСсти ΠΈ ΡƒΠ΄Π»ΠΈΠ½Π΅Π½ΠΈΠ΅ лишь 54 ΠΈ 43% соотвСтствСнно для основного ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°. ПослС мСТкристаллитной ΠΊΠΎΡ€Ρ€ΠΎΠ·ΠΈΠΈ ΠΌΠΈΠΊΡ€ΠΎΡ‚Π²Π΅Ρ€Π΄ΠΎΡΡ‚ΡŒ явно измСняСтся, ΠΈ коррозионная ΡΡ‚ΠΎΠΉΠΊΠΎΡΡ‚ΡŒ Π½ΠΈΠΆΠ΅ Ρƒ основания Π·ΠΎΠ½Ρ‹ ядра сварной Ρ‚ΠΎΡ‡ΠΊΠΈ. Π’ Π·ΠΎΠ½Π΅ ядра сварной Ρ‚ΠΎΡ‡ΠΊΠΈ ΠΈ Π½Π° повСрхности Π½Π΅ Π½Π°Π±Π»ΡŽΠ΄Π°Π΅Ρ‚ΡΡ измСнСния микротвСрдости, хотя ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ микротвСрдости явно Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½ΠΎ, Π° коррозионная ΡΡ‚ΠΎΠΉΠΊΠΎΡΡ‚ΡŒ Π½ΠΈΠΆΠ΅ Π² Π·ΠΎΠ½Π°Ρ… тСрмомСханичСского ΠΈ тСрмичСского влияния

    Structure-properties relationships in solution-processable single-material molecular emitters for efficient green organic light-emitting diodes

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    The electroluminescent properties of a series of solution-processable fluorescent molecular emitters have been systematically investigated. While the introduction of the electron-deficient benzothiadiazole unit in the structure confers efficient electron-injection on the emitter materials, they exhibit different hole-transport properties. The device characteristics of the OLEDs based on these various emitters are discussed on the basis of (i) the energy levels of their HOMO and LUMO and (ii) their hole-transport properties in relation with the charge-transport and blocking properties of the electron- and hole-transport layers. (C) 2012 Elsevier B.V. All rights reserved

    First-in-class Microbial Ecosystem Therapeutic 4 (MET4) in combination with immune checkpoint inhibitors in patients with advanced solid tumors (MET4-IO trial)

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    Background: The intestinal microbiome has been associated with response to immune checkpoint inhibitors (ICIs) in humans and causally implicated in ICI responsiveness in animal models. Two recent human trials demonstrated that fecal microbiota transplant (FMT) from ICI responders can rescue ICI responses in refractory melanoma, but FMT has specific limitations to scaled use.Patients and methods: We conducted an early-phase clinical trial of a cultivated, orally delivered 30-species microbial consortium (Microbial Ecosystem Therapeutic 4, MET4) designed for co-administration with ICIs as an alternative to FMT and assessed safety, tolerability and ecological responses in patients with advanced solid tumors.Results: The trial achieved its primary safety and tolerability outcomes. There were no statistically significant differences in the primary ecological outcomes; however, differences in MET4 species relative abundance were evident after randomization that varied by patient and species. Increases in the relative abundance of several MET4 taxa, including Enterococcus and Bifidobacterium, taxa previously associated with ICI responsiveness, were observed and MET4 engraftment was associated with decreases in plasma and stool primary bile acids.Conclusions: This trial is the first report of the use of a microbial consortium as an alternative to FMT in advanced cancer patients receiving ICI and the results justify the further development of microbial consortia as a therapeutic co-intervention for ICI treatment in cancer

    Partial wave analysis of J/\psi \to \gamma \phi \phi

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    Using 5.8Γ—107J/ψ5.8 \times 10^7 J/\psi events collected in the BESII detector, the radiative decay J/Οˆβ†’Ξ³Ο•Ο•β†’Ξ³K+Kβˆ’KS0KL0J/\psi \to \gamma \phi \phi \to \gamma K^+ K^- K^0_S K^0_L is studied. The ϕϕ\phi\phi invariant mass distribution exhibits a near-threshold enhancement that peaks around 2.24 GeV/c2c^{2}. A partial wave analysis shows that the structure is dominated by a 0βˆ’+0^{-+} state (Ξ·(2225)\eta(2225)) with a mass of 2.24βˆ’0.02+0.03βˆ’0.02+0.032.24^{+0.03}_{-0.02}{}^{+0.03}_{-0.02} GeV/c2c^{2} and a width of 0.19Β±0.03βˆ’0.04+0.060.19 \pm 0.03^{+0.06}_{-0.04} GeV/c2c^{2}. The product branching fraction is: Br(J/Οˆβ†’Ξ³Ξ·(2225))β‹…Br(Ξ·(2225)→ϕϕ)=(4.4Β±0.4Β±0.8)Γ—10βˆ’4Br(J/\psi \to \gamma \eta(2225))\cdot Br(\eta(2225)\to \phi\phi) = (4.4 \pm 0.4 \pm 0.8)\times 10^{-4}.Comment: 11 pages, 4 figures. corrected proof for journa

    Measurements of the observed cross sections for e+eβˆ’β†’e^+e^-\to exclusive light hadrons containing Ο€0Ο€0\pi^0\pi^0 at s=3.773\sqrt s= 3.773, 3.650 and 3.6648 GeV

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    By analyzing the data sets of 17.3, 6.5 and 1.0 pbβˆ’1^{-1} taken, respectively, at s=3.773\sqrt s= 3.773, 3.650 and 3.6648 GeV with the BES-II detector at the BEPC collider, we measure the observed cross sections for e+eβˆ’β†’Ο€+Ο€βˆ’Ο€0Ο€0e^+e^-\to \pi^+\pi^-\pi^0\pi^0, K+Kβˆ’Ο€0Ο€0K^+K^-\pi^0\pi^0, 2(Ο€+Ο€βˆ’Ο€0)2(\pi^+\pi^-\pi^0), K+Kβˆ’Ο€+Ο€βˆ’Ο€0Ο€0K^+K^-\pi^+\pi^-\pi^0\pi^0 and 3(Ο€+Ο€βˆ’)Ο€0Ο€03(\pi^+\pi^-)\pi^0\pi^0 at the three energy points. Based on these cross sections we set the upper limits on the observed cross sections and the branching fractions for ψ(3770)\psi(3770) decay into these final states at 90% C.L..Comment: 7 pages, 2 figure

    Direct Measurements of Absolute Branching Fractions for D0 and D+ Inclusive Semimuonic Decays

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    By analyzing about 33 pbβˆ’1\rm pb^{-1} data sample collected at and around 3.773 GeV with the BES-II detector at the BEPC collider, we directly measure the branching fractions for the neutral and charged DD inclusive semimuonic decays to be BF(D0β†’ΞΌ+X)=(6.8Β±1.5Β±0.7)BF(D^0 \to \mu^+ X) =(6.8\pm 1.5\pm 0.7)% and BF(D+β†’ΞΌ+X)=(17.6Β±2.7Β±1.8)BF(D^+ \to \mu^+ X) =(17.6 \pm 2.7 \pm 1.8)%, and determine the ratio of the two branching fractions to be BF(D+β†’ΞΌ+X)BF(D0β†’ΞΌ+X)=2.59Β±0.70Β±0.25\frac{BF(D^+ \to \mu^+ X)}{BF(D^0 \to \mu^+ X)}=2.59\pm 0.70 \pm 0.25

    Direct Measurements of the Branching Fractions for D0β†’Kβˆ’e+Ξ½eD^0 \to K^-e^+\nu_e and D0β†’Ο€βˆ’e+Ξ½eD^0 \to \pi^-e^+\nu_e and Determinations of the Form Factors f+K(0)f_{+}^{K}(0) and f+Ο€(0)f^{\pi}_{+}(0)

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    The absolute branching fractions for the decays D0β†’Kβˆ’e+Ξ½eD^0 \to K^-e ^+\nu_e and D0β†’Ο€βˆ’e+Ξ½eD^0 \to \pi^-e^+\nu_e are determined using 7584Β±198Β±3417584\pm 198 \pm 341 singly tagged DΛ‰0\bar D^0 sample from the data collected around 3.773 GeV with the BES-II detector at the BEPC. In the system recoiling against the singly tagged DΛ‰0\bar D^0 meson, 104.0Β±10.9104.0\pm 10.9 events for D0β†’Kβˆ’e+Ξ½eD^0 \to K^-e ^+\nu_e and 9.0Β±3.69.0 \pm 3.6 events for D0β†’Ο€βˆ’e+Ξ½eD^0 \to \pi^-e^+\nu_e decays are observed. Those yield the absolute branching fractions to be BF(D0β†’Kβˆ’e+Ξ½e)=(3.82Β±0.40Β±0.27)BF(D^0 \to K^-e^+\nu_e)=(3.82 \pm 0.40\pm 0.27)% and BF(D0β†’Ο€βˆ’e+Ξ½e)=(0.33Β±0.13Β±0.03)BF(D^0 \to \pi^-e^+\nu_e)=(0.33 \pm 0.13\pm 0.03)%. The vector form factors are determined to be ∣f+K(0)∣=0.78Β±0.04Β±0.03|f^K_+(0)| = 0.78 \pm 0.04 \pm 0.03 and ∣f+Ο€(0)∣=0.73Β±0.14Β±0.06|f^{\pi}_+(0)| = 0.73 \pm 0.14 \pm 0.06. The ratio of the two form factors is measured to be ∣f+Ο€(0)/f+K(0)∣=0.93Β±0.19Β±0.07|f^{\pi}_+(0)/f^K_+(0)|= 0.93 \pm 0.19 \pm 0.07.Comment: 6 pages, 5 figure

    A study of charged kappa in J/Οˆβ†’KΒ±KsΟ€βˆ“Ο€0J/\psi \to K^{\pm} K_s \pi^{\mp} \pi^0

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    Based on 58Γ—10658 \times 10^6 J/ψJ/\psi events collected by BESII, the decay J/Οˆβ†’KΒ±KsΟ€βˆ“Ο€0J/\psi \to K^{\pm} K_s \pi^{\mp} \pi^0 is studied. In the invariant mass spectrum recoiling against the charged Kβˆ—(892)Β±K^*(892)^{\pm}, the charged ΞΊ\kappa particle is found as a low mass enhancement. If a Breit-Wigner function of constant width is used to parameterize the kappa, its pole locates at (849Β±77βˆ’14+18)βˆ’i(256Β±40βˆ’22+46)(849 \pm 77 ^{+18}_{-14}) -i (256 \pm 40 ^{+46}_{-22}) MeV/c2c^2. Also in this channel, the decay J/Οˆβ†’Kβˆ—(892)+Kβˆ—(892)βˆ’J/\psi \to K^*(892)^+ K^*(892)^- is observed for the first time. Its branching ratio is (1.00Β±0.19βˆ’0.32+0.11)Γ—10βˆ’3(1.00 \pm 0.19 ^{+0.11}_{-0.32}) \times 10^{-3}.Comment: 14 pages, 4 figure
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