866 research outputs found

    Energy States of Colored Particle in a Chromomagnetic Field

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    The unitary transformation, which diagonalizes squared Dirac equation in a constant chromomagnetic field is found. Applying this transformation, we find the eigenfunctions of diagonalized Hamiltonian, that describe the states with definite value of energy and call them energy states. It is pointed out that, the energy states are determined by the color interaction term of the particle with the background chromofield and this term is responsible for the splitting of the energy spectrum. We construct supercharge operators for the diagonal Hamiltonian, that ensure the superpartner property of the energy states.Comment: 25 pages, some calculation details have been removed, typos correcte

    The indisputable value of ultrasound diagnostics in acute small bowel obstruction

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    The use of ultrasound in the diagnosis of acute small bowel obstruction is justified from a tactical point of view, since it is not delayed in time, does not weigh down the patient's condition, has sufficient information and does not carry radiation load. Due to its safety and ease of use, this technique can be used repeatedly in the process of conservative treatment to determine further treatment tactics

    Condensation of 4-hydroxy-2-thiazolines with 1,2-phenylenediamine as a novel effective route to thiazolo[3,4-a]quinoxalines

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    Thiazolo[3,4-a]quinoxalin-4-ones were prepared in two steps starting from methyl phenylchloropyruvate using a new strategy for the construction of the ring system. A key step in this new method involves the reaction of 4-hydroxytetrahydrothiazoles with 1,2-phenylendiamines

    Study of regularities on how drilling cuttings block pores and fractures of oil-bearing formation

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    Regularities on how drilling cuttings block pores and fractures of oil-bearing formation are studied. There are complex physical and chemical processes at well bottomhole occur during entering oil-bearing formation by rotary or rope drilling. That is caused by quality of drilling fluid, intensity of washing, rotation of a drill string, presence of cuttings at bottomhole and a drilling technique. There are hydraulic impulse effects with alternating signs in bottomhole formation zone appear during rope drilling that have a significant impact on quality of work. Underestimation of mentioned factors during entering oil-bearing reservoirs leads to decrease in permeability of oil rocks and well production rate. A clear understanding of physical and chemical processes at bottomhole while entering oil-bearing reservoirs and management of these processes allow to avoid reduce in conductivity of reservoir rocks to a large extent and intensify it in some cases. The main conditions to increase efficiency of oil wells drilling are application of such methods of entering and development of an oil-bearing reservoir that ensure preservation of its natural porosity and permeability or contribute to their increase in bottomhole part of a well. Physical and chemical parameters of oil-bearing formation are the governing factor while choosing its entering and development technology. In recent years, great attention has been paid to issues of entering and development oil reservoirs. Parameters such as geological and physical properties of a reservoir, physical and chemical properties of reservoir oil, rocks and washing liquid, hydrodynamic interaction in an "oil reservoir-well" system are not considered enough in a number of cases during entering and development of a formation. That often leads to incorrect conclusions about a possibility to use actual reserves for needs of national economy. Drilling of oil-bearing formations is a technological process, which create a bore hole in a productive oil-bearing formation for equipment of oil part of a well. Bringing a well on production include technological operations that provide installation of equipment into an oil part of a well and restoration of natural oil permeability of a formation or its artificial increase to achieve maximum production rate of a well

    Unoccupied Topological States on Bismuth Chalcogenides

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    The unoccupied part of the band structure of topological insulators Bi2_2Tex_{x}Se3βˆ’x_{3-x} (x=0,2,3x=0,2,3) is studied by angle-resolved two-photon photoemission and density functional theory. For all surfaces linearly-dispersing surface states are found at the center of the surface Brillouin zone at energies around 1.3 eV above the Fermi level. Theoretical analysis shows that this feature appears in a spin-orbit-interaction induced and inverted local energy gap. This inversion is insensitive to variation of electronic and structural parameters in Bi2_2Se3_3 and Bi2_2Te2_2Se. In Bi2_2Te3_3 small structural variations can change the character of the local energy gap depending on which an unoccupied Dirac state does or does not exist. Circular dichroism measurements confirm the expected spin texture. From these findings we assign the observed state to an unoccupied topological surface state

    Opening of a pseudogap in a quasi-two dimensional superconductor due to critical thermal fluctuations

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    We examine the role of the anisotropy of superconducting critical thermal fluctuations in the opening of a pseudogap in a quasi-two dimensional superconductor such as a cuprate-oxide high-temperature superconductor. When the anisotropy between planes and their perpendicular axis is large enough and its superconducting critical temperature T_c is high enough, the fluctuations are much developed in its critical region so that lifetime widths of quasiparticles are large and the energy dependence of the selfenergy deviates from that of Landau's normal Fermi liquids. A pseudogap opens in such a critical region because quasiparticle spectra around the chemical potential are swept away due to the large lifetime widths. The pseudogap never smoothly evolves into a superconducting gap; it starts to open at a temperature higher than T_c while the superconducting gap starts to open just at T_c. When T_c is rather low but the ratio of varepsilon_G(0)/k_BT_c, with varepsilon_G(0) the superconducting gap at T=0K and k_B the Boltzmann constant, is much larger than a value about 4 according to the mean-field theory, the pseudogap must be closing as temperature T approaches to the low T_c because thermal fluctuations become less developed as T decreases. Critical thermal fluctuations cannot cause the opening of a prominent pseudogap in an almost isotropic three dimensional superconductor, even if its T_c is high.Comment: 25 pages, 5 figures (14 subfigures

    ΠžΡ†Π΅Π½ΠΊΠ° эффСктивности ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ примСнСния способов ΠΏΡ€ΠΎΡ„ΠΈΠ»Π°ΠΊΡ‚ΠΈΠΊΠΈ Π½Π΅ΡΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ швов ΠΊΠΈΡˆΠ΅Ρ‡Π½Ρ‹Ρ… анастомозов

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    ЦСль. Π˜Π·ΡƒΡ‡Π΅Π½ΠΈΠ΅ эффСктивности ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… способов ΠΏΡ€ΠΎΡ„ΠΈΠ»Π°ΠΊΡ‚ΠΈΠΊΠΈ Π½Π΅ΡΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ швов ΠΊΠΈΡˆΠ΅Ρ‡Π½Ρ‹Ρ… анастомозов (НШКА) Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… послС ΠΏΠ»Π°Π½ΠΎΠ²ΠΎΠΉ, экстрСнной ΠΈ Π½Π΅ΠΎΡ‚Π»ΠΎΠΆΠ½ΠΎΠΉ Ρ€Π΅Π·Π΅ΠΊΡ†ΠΈΠΈ Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… сСгмСнтов ΠΊΠΈΡˆΠ΅Ρ‡Π½ΠΈΠΊΠ°. ΠœΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Ρ‹ ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹. Π˜Π·ΡƒΡ‡Π΅Π½ΠΎ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ лСчСния 642 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹ΠΌ Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° рСзСкция Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… сСгмСнтов Ρ‚ΠΎΠ½ΠΊΠΎΠΉ ΠΈ толстой кишок с Π½Π°Π»ΠΎΠΆΠ΅Π½ΠΈΠ΅ΠΌ ΠΏΠ΅Ρ€Π²ΠΈΡ‡Π½Ρ‹Ρ… анастомозов. Из 642 Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… 357 (55,6%) ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Ρ‹ Π² ΠΏΠ»Π°Π½ΠΎΠ²ΠΎΠΌ порядкС, 285 (44,4%) - ΠΏΠΎ Π½Π΅ΠΎΡ‚Π»ΠΎΠΆΠ½Ρ‹ΠΌ ΠΈ экстрСнным показаниям. Π£ 467 (72,7%) Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… Π½Π°Π»ΠΎΠΆΠ΅Π½Ρ‹ анастомозы ΠΏΠΎ Ρ‚ΠΈΠΏΡƒ Π±ΠΎΠΊ Π² Π±ΠΎΠΊ, Ρƒ 150 (23,4%) - ΠΏΠΎ Ρ‚ΠΈΠΏΡƒ ΠΊΠΎΠ½Π΅Ρ† Π² ΠΊΠΎΠ½Π΅Ρ†, Ρƒ 25 (3,8%) - ΠΏΠΎ Ρ‚ΠΈΠΏΡƒ ΠΊΠΎΠ½Π΅Ρ† Π² Π±ΠΎΠΊ. Π‘ Ρ†Π΅Π»ΡŒΡŽ ΠΏΡ€ΠΎΡ„ΠΈΠ»Π°ΠΊΡ‚ΠΈΠΊΠΈ НШКА выполняли ΠΏΠ΅Ρ€ΠΌΠ°Π½Π΅Π½Ρ‚Π½ΡƒΡŽ Π²Π½ΡƒΡ‚Ρ€ΠΈΠ±Ρ€Ρ‹ΠΆΠ΅Π΅Ρ‡Π½ΡƒΡŽ Π±Π»ΠΎΠΊΠ°Π΄Ρƒ, ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Π»ΠΈΠΌΡ„ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΡƒΡŽ Ρ‚Π΅Ρ€Π°ΠΏΠΈΡŽ, ΠΌΠ΅ΡΡ‚Π½ΡƒΡŽ Π»Π°Π·Π΅Ρ€ΠΎΠΌΠ°Π³Π½ΠΈΡ‚ΠΎΡ‚Π΅Ρ€Π°ΠΏΠΈΡŽ, ΠΈΠ½Ρ‚ΡƒΠ±Π°Ρ†ΠΈΠΎΠ½Π½ΡƒΡŽ Π΄Π΅ΠΊΠΎΠΌΠΏΡ€Π΅ΡΡΠΈΡŽ, ΡΠ°Π½Π°Ρ†ΠΈΡŽ ΠΈ Π³Π°ΡΡ‚Ρ€ΠΎΡΠ½Ρ‚Π΅Ρ€ΠΎΡΠΎΡ€Π±Ρ†ΠΈΡŽ с ΠΏΠΎΠ»ΠΈΡ„Π΅ΠΏΠ°Π½ΠΎΠΌ, Π° Ρ‚Π°ΠΊΠΆΠ΅ Π²Π½ΡƒΡ‚Ρ€ΠΈΠΌΡ‹ΡˆΠ΅Ρ‡Π½ΠΎ Π²Π²ΠΎΠ΄ΠΈΠ»ΠΈ чСловСчСский ΠΏΠ»Π°Ρ†Π΅Π½Ρ‚Π°Ρ€Π½Ρ‹ΠΉ Π³ΠΈΠ΄Ρ€ΠΎΠ»ΠΈΠ·Π°Ρ‚ Β«LaennecΒ». Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. НШКА наблюдали Ρƒ 10 (1,6%) Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…: Ρƒ 6 (4,0%) - с анастомозами ΠΊΠΎΠ½Π΅Ρ† Π² ΠΊΠΎΠ½Π΅Ρ† ΠΈ Ρƒ 4 (0,86%) - с анастомозами Π±ΠΎΠΊ Π² Π±ΠΎΠΊ. ΠΠ΅ΡΠΎΡΡ‚ΠΎΡΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π±Ρ‹Π»ΠΈ 1 (10%) Ρ‚ΠΎΠ½ΠΊΠΎ-Ρ‚ΠΎΠ»ΡΡ‚ΠΎΠΊΠΈΡˆΠ΅Ρ‡Π½Ρ‹ΠΉ анастомоз, 2 (20%) Ρ‚ΠΎΠ½ΠΊΠΎ-Ρ‚ΠΎΠ½ΠΊΠΎΠΊΠΈΡˆΠ΅Ρ‡Π½Ρ‹Ρ… ΠΈ 7 (70%) толсто-Ρ‚ΠΎΠ»ΡΡ‚ΠΎΠΊΠΈΡˆΠ΅Ρ‡Π½Ρ‹Ρ… анастомозов. Π’Ρ‹Π²ΠΎΠ΄Ρ‹. Π‘ Ρ†Π΅Π»ΡŒΡŽ ΠΏΡ€ΠΎΡ„ΠΈΠ»Π°ΠΊΡ‚ΠΈΠΊΠΈ НШКА Ρƒ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ…, ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π² Π½Π΅ΠΎΡ‚Π»ΠΎΠΆΠ½ΠΎΠΌ, экстрСнном ΠΈ ΠΏΠ»Π°Π½ΠΎΠ²ΠΎΠΌ порядкС, рСкомСндуСтся ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΠΎΠ²Π°Ρ‚ΡŒ ΠΏΠΎ показаниям ΠΏΠ΅Ρ€ΠΌΠ°Π½Π΅Π½Ρ‚Π½ΡƒΡŽ Π²Π½ΡƒΡ‚Ρ€ΠΈΠ±Ρ€Ρ‹ΠΆΠ΅Π΅Ρ‡Π½ΡƒΡŽ (Π·Π°Π±Ρ€ΡŽΡˆΠΈΠ½Π½ΡƒΡŽ) Π±Π»ΠΎΠΊΠ°Π΄Ρƒ с Π»ΠΈΠΌΡ„ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠΉ Ρ‚Π΅Ρ€Π°ΠΏΠΈΠ΅ΠΉ, ΠΌΠ΅ΡΡ‚Π½ΡƒΡŽ Π»Π°Π·Π΅Ρ€ΠΎΠΌΠ°Π³Π½ΠΈΡ‚ΠΎΡ‚Π΅Ρ€Π°ΠΏΠΈΡŽ, ΠΈΠ½Ρ‚ΡƒΠ±Π°Ρ†ΠΈΠΎΠ½Π½ΡƒΡŽ Π΄Π΅ΠΊΠΎΠΌΠΏΡ€Π΅ΡΡΠΈΡŽ, ΡΠ°Π½Π°Ρ†ΠΈΡŽ ΠΈ Π³Π°ΡΡ‚Ρ€ΠΎΡΠ½Ρ‚Π΅Ρ€ΠΎΡΠΎΡ€Π±Ρ†ΠΈΡŽ с ΠΏΠΎΠ»ΠΈΡ„Π΅ΠΏΠ°Π½ΠΎΠΌ, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΡ€Π΅ΠΏΠ°Ρ€Π°Ρ‚ Β«Laennec
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