1,256 research outputs found

    Development of dysbiosis in the organism of rats receiving a high-fat diet

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    Background. To determine the effect on the degree of dysbiosis in the organs and tissues of rats treated with high-fat diet (HFD) using fats with various fatty acid compositions.Methods. We used ordinary (high-linoleic) sunflower oil, high-oleic sunflower oil, butter, palm and coconut oils. Rats were fed with 15 % of each of the fats for 64 days. In the blood serum from v.cava and v. porta, in the liver, heart, brain, skeletal muscles and intestinal mucosa, urease activity (an indicator of bacterial insemination), lysozyme activity (a factor of non-specific immunity) were determined, and the degree of dysbiosis was calculated from the ratio of relative urease and lysozyme activities.Β Results. The activity of urease in the blood of v. porta increased in rats treated with HFD, and was significantly higher than in the blood of v.cava. In most of the studied tissues, urease activity increased after HFD, with the exception of rats receiving high-oleic sunflower oil (HOSO). In contrast, lysozyme activity was reduced in most tissues, with the exception of rats treated with HOSO. The degree of dysbiosis increased after HFD with the exception of rats treated with HOSO.Conclusion. HFD increases the translocation of bacteria from the intestine. The liver partially neutralizes the microflora coming from the intestines. In blood serum from v. cava and v. porta, urease activity (an indicator of bacterial contamination), lysozyme activity (nonspecific immunity factor) were determined in the liver, heart, brain, skeletal muscle and intestinal mucosa, and the degree of dysbiosis was calculated by the ratio of the relative activities of urease and lysozyme.Results. Blood urease activity v. porta was elevated in rats treated with HFD and was significantly higher than in blood v. cava. In most of the tissues studied, urease activity increased after HFD with the exception of rats treated with high oleic sunflower oil (HOSO), the development of dysbiosis in all tissues of the body. The exception is HOSO, which does not cause the development of dysbiosis and inflammation

    Hadron and Quark Form Factors in the Relativistic Harmonic Oscillator Model

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    Nucleon, pion and quark form factors are studied within the relativistic harmonic oscillator model including the quark spin. It is shown that the nucleon charge, magnetic and axial form factors and the pion charge form factor can be explained with one oscillator parameter if one accounts for the scaling rule and the size of the constituent quarks.Comment: 9 pages, Latex, 3 postscript figures, DFTT 8/9

    The Boltzmann equation for colourless plasmons in hot QCD plasma. Semiclassical approximation

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    Within the framework of the semiclassical approximation, we derive the Boltzmann equation describing the dynamics of colorless plasmons in a hot QCD plasma. The probability of the plasmon-plasmon scattering at the leading order in the coupling constant is obtained. This probability is gauge-independent at least in the class of the covariant and temporal gauges. It is noted that the structure of the scattering kernel possesses important qualitative difference from the corresponding one in the Abelian plasma, in spite of the fact that we focused our study on the colorless soft excitations. It is shown that four-plasmon decay is suppressed by the power of gg relative to the process of nonlinear scattering of plasmons by thermal particles at the soft momentum scale. It is stated that the former process becomes important in going to the ultrasoft region of the momentum scale.Comment: 41, LaTeX, minor changes, identical to published versio

    Spiral Growth and Step Edge Barriers

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    The growth of spiral mounds containing a screw dislocation is compared to the growth of wedding cakes by two-dimensional nucleation. Using phase field simulations and homoepitaxial growth experiments on the Pt(111) surface we show that both structures attain the same characteristic large scale shape when a significant step edge barrier suppresses interlayer transport. The higher vertical growth rate observed for the spiral mounds on Pt(111) reflects the different incorporation mechanisms for atoms in the top region and can be formally represented by an enhanced apparent step edge barrier.Comment: 11 pages, 4 figures, partly in colo

    Parity violating cylindrical shell in the framework of QED

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    We present calculations of Casimir energy (CE) in a system of quantized electromagnetic (EM) field interacting with an infinite circular cylindrical shell (which we call `the defect'). Interaction is described in the only QFT-consistent way by Chern-Simon action concentrated on the defect, with a single coupling constant aa. For regularization of UV divergencies of the theory we use % physically motivated Pauli-Villars regularization of the free EM action. The divergencies are extracted as a polynomial in regularization mass MM, and they renormalize classical part of the surface action. We reveal the dependence of CE on the coupling constant aa. Corresponding Casimir force is attractive for all values of aa. For aβ†’βˆža\to\infty we reproduce the known results for CE for perfectly conducting cylindrical shell first obtained by DeRaad and Milton.Comment: Typos corrected. Some references adde

    A Cosmological Theory without Singularities

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    A theory of gravitation is constructed in which all homogeneous and isotropic solutions are nonsingular, and in which all curvature invariants are bounded. All solutions for which curvature invariants approach their limiting values approach de Sitter space. The action for this theory is obtained by a higher derivative modification of Einstein's theory. We expect that our model can easily be generalized to solve the singularity problem also for anisotropic cosmologies.Comment: 25 pages, 11 figures (available as hard copies from the authors), uses phyzzx, BROWN-HET-89

    Measurements of light background at large depth in the ocean

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    The mean intensity of Cerenkov emission from the products of K(40) decay and bioluminescence was measured at depths to 5 km. The intensity of ocean light background is found to depend upon depth and at the 5 km level is equal on averaged to 300 + or - 60 quanta/sq cms into spatial angle of 2 pi sterradian in transparency window. The amplitudes, duration and number of BL flashes were measured at various depths. The intensive flashes due to BL are shown to be observed rather seldom at depths over 4 km

    Взаємодія 4,5-Π΄ΠΈΡ„ΠΎΡ€ΠΌΡ–Π»-2,3,6,7,8,10-гСксагідроакридин-8Π°(1Н)-ΠΊΠ°Ρ€Π±ΠΎΠ½Ρ–Ρ‚Ρ€ΠΈΠ»Ρƒ Π· N-Π½ΡƒΠΊΠ»Π΅ΠΎΡ„Ρ–Π»Π°ΠΌΠΈ

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    Schiff bases are of practical interest as initial materials both for the combinatorial synthesis for libraries of compounds, and for preparation of complexes with metals; thus, currently the intensity of research in this direction is increasing. The possibilities of practical use of complex compounds with organic ligands are quite broad varying from effective catalysts of various chemical processes to molecular sensors. While studying formylation of 5,6,7,8-tetrahydro-1H-spiro[cyclohexane-1,2-quinazolin]-4’(3’H)-one a new domino reaction, which makes it possible to obtain tricyclic acridine systems, has been carried out. In spite of the reduced electrophilicity of the aldehyde groups in 4,5-diformyl-2,3,6,7,8,10-hexahydroacridine-8Π°(1H)-carbonitrile the latter is shown to react with various amines in benzene with azeotropic removal of water using p-TsOH as a catalyst, and with hydroxylamine hydrochloride in i-PrOH. New Schiff bases and oxime obtained are of potential interest as ligands for formation of chelate complexes. The reaction of dialdehyde with N2H4Γ—H2O instead of the expected hydrazone resulted in obtaining a macrocyclic compound – a derivative of hexaazacyclooctadecine. The structure of the compounds obtained corresponds to the data of 1H NMR-spectroscopy, mass spectrometry and elemental analysis. The preliminary studies have shown that azomethines – 4,5-phenyl(cyclohexcyl)iminomethyl-2,3,6,7,8,10-hexahydroacridine8Π°(1H)-carbonitrile create complexes with copper and nickel ions.Основания Π¨ΠΈΡ„Ρ„Π° ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ практичСский интСрСс Π² качСствС исходных ΠΊΠ°ΠΊ для ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ‚ΠΎΡ€Π½ΠΎΠ³ΠΎ синтСза Π±ΠΈΠ±Π»ΠΈΠΎΡ‚Π΅ΠΊ вСщСств, Ρ‚Π°ΠΊ ΠΈ для создания комплСксов с ΠΌΠ΅Ρ‚Π°Π»Π»Π°ΠΌΠΈ, ΠΈ Π² послСднСС врСмя ΠΈΠ½Ρ‚Π΅Π½ΡΠΈΠ²Π½ΠΎΡΡ‚ΡŒ исслСдований Π² Π΄Π°Π½Π½ΠΎΠΌ Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ увСличиваСтся. ВозмоТности практичСского использования комплСксных соСдинСний с органичСскими Π»ΠΈΠ³Π°Π½Π΄Π°ΠΌΠΈ вСсьма ΡˆΠΈΡ€ΠΎΠΊΠΈ: ΠΎΡ‚ эффСктивных ΠΊΠ°Ρ‚Π°Π»ΠΈΠ·Π°Ρ‚ΠΎΡ€ΠΎΠ² Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… химичСских процСссов Π΄ΠΎ молСкулярных сСнсоров. Π’ Ρ…ΠΎΠ΄Π΅ изучСния формилирования 5’,6’,7’,8’-Ρ‚Π΅Ρ‚Ρ€Π°Π³ΠΈΠ΄Ρ€ΠΎ-1’Н-спиро[циклогСксан-1,2’-Ρ…ΠΈΠ½Π°Π·ΠΎΠ»ΠΈΠ½]-4’(3’Н)-ΠΎΠ½Π° Π½Π°ΠΌΠΈ Π±Ρ‹Π»Π° Π½Π°ΠΉΠ΄Π΅Π½Π° новая Π΄ΠΎΠΌΠΈΠ½ΠΎ-рСакция, которая позволяСт Π²Ρ‹ΠΉΡ‚ΠΈ Π½Π° трицикличСскиС Π³ΠΈΠ΄Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Π΅ Π°ΠΊΡ€ΠΈΠ΄ΠΈΠ½ΠΎΠ²Ρ‹Π΅ систСмы. Показано, Ρ‡Ρ‚ΠΎ нСсмотря Π½Π° ΡΠ½ΠΈΠΆΠ΅Π½Π½ΡƒΡŽ ΡΠ»Π΅ΠΊΡ‚Ρ€ΠΎΡ„ΠΈΠ»ΡŒΠ½ΠΎΡΡ‚ΡŒ Π°Π»ΡŒΠ΄Π΅Π³ΠΈΠ΄Π½Ρ‹Ρ… Π³Ρ€ΡƒΠΏΠΏ Π² 4,5-Π΄ΠΈΡ„ΠΎΡ€ΠΌΠΈΠ»2,3,6,7,8,10-гСксагидроакридин-8Π°(1Н)-ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΈΡ‚Ρ€ΠΈΠ»Π΅, ΠΎΠ½ Ρ€Π΅Π°Π³ΠΈΡ€ΡƒΠ΅Ρ‚ с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ Π°ΠΌΠΈΠ½Π°ΠΌΠΈ Π² Π±Π΅Π½Π·ΠΎΠ»Π΅ с Π°Π·Π΅ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΠΉ ΠΎΡ‚Π³ΠΎΠ½ΠΊΠΎΠΉ Π²ΠΎΠ΄Ρ‹ с ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π² качСствС ΠΊΠ°Ρ‚Π°Π»ΠΈΠ·Π°Ρ‚ΠΎΡ€Π° p-TsOH, Π° Ρ‚Π°ΠΊΠΆΠ΅ с солянокислым гидроксиламином Π² i-PrOH. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ основания Π¨ΠΈΡ„Ρ„Π° ΠΈ оксим ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΉ интСрСс Π² качСствС Π»ΠΈΠ³Π°Π½Π΄ΠΎΠ² для образования Ρ…Π΅Π»Π°Ρ‚Π½Ρ‹Ρ… комплСксов. Π’ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ Ρ€Π΅Π°ΠΊΡ†ΠΈΠΈ диальдСгида с N2H4Γ—H2O вмСсто ΠΎΠΆΠΈΠ΄Π°Π΅ΠΌΠΎΠ³ΠΎ Π³ΠΈΠ΄Ρ€Π°Π·ΠΎΠ½Π° ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΎ макроцикличСскоС соСдинСниС – ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΠΎΠ΅ гСксаазациклооктадСцина. Π‘Ρ‚Ρ€ΠΎΠ΅Π½ΠΈΠ΅ всСх ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… соСдинСний согласуСтся с Π΄Π°Π½Π½Ρ‹ΠΌΠΈ ЯМР 1Н-спСктроскопии, масс-спСктромСтрии ΠΈ элСмСнтного Π°Π½Π°Π»ΠΈΠ·Π°. ΠŸΡ€Π΅Π΄Π²Π°Ρ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ исслСдования ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ Π°Π·ΠΎΠΌΠ΅Ρ‚ΠΈΠ½Ρ‹ βˆ’ 4,5-Ρ„Π΅Π½ΠΈΠ»(циклогСксил)ΠΈΠΌΠΈΠ½ΠΎΠΌΠ΅Ρ‚ΠΈΠ»-2,3,6,7,8,10-гСксагидроакридин-8Π°(1Н)ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΈΡ‚Ρ€ΠΈΠ»Π° ΠΎΠ±Ρ€Π°Π·ΡƒΡŽΡ‚ комплСксныС соСдинСния с ΠΈΠΎΠ½Π°ΠΌΠΈ никСля ΠΈ ΠΌΠ΅Π΄ΠΈ. Основи Π¨ΠΈΡ„Ρ„Π° ΡΡ‚Π°Π½ΠΎΠ²Π»ΡΡ‚ΡŒ ΠΏΡ€Π°ΠΊΡ‚ΠΈΡ‡Π½ΠΈΠΉ інтСрСс Π² якості Π²ΠΈΡ…Ρ–Π΄Π½ΠΈΡ… як для ΠΊΠΎΠΌΠ±Ρ–Π½Π°Ρ‚ΠΎΡ€Π½ΠΎΠ³ΠΎ синтСзу Π±Ρ–Π±Π»Ρ–ΠΎΡ‚Π΅ΠΊ Ρ€Π΅Ρ‡ΠΎΠ²ΠΈΠ½, Ρ‚Π°ΠΊ Ρ– для створСння комплСксів Π· ΠΌΠ΅Ρ‚Π°Π»Π°ΠΌΠΈ, Ρ– останнім часом Ρ–Π½Ρ‚Π΅Π½ΡΠΈΠ²Π½Ρ–ΡΡ‚ΡŒ Π΄ΠΎΡΠ»Ρ–Π΄ΠΆΠ΅Π½ΡŒ Ρƒ Π΄Π°Π½ΠΎΠΌΡƒ напрямку Ρ‚Ρ–Π»ΡŒΠΊΠΈ Π·Π±Ρ–Π»ΡŒΡˆΡƒΡ”Ρ‚ΡŒΡΡ. ΠœΠΎΠΆΠ»ΠΈΠ²ΠΎΡΡ‚Ρ– ΠΏΡ€Π°ΠΊΡ‚ΠΈΡ‡Π½ΠΎΠ³ΠΎ використання комплСксів Π· ΠΎΡ€Π³Π°Π½Ρ–Ρ‡Π½ΠΈΠΌΠΈ Π»Ρ–Π³Π°Π½Π΄Π°ΠΌΠΈ Π΄ΠΎΡΠΈΡ‚ΡŒ ΡˆΠΈΡ€ΠΎΠΊΡ–: Π²Ρ–Π΄ Π΅Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΈΡ… ΠΊΠ°Ρ‚Π°Π»Ρ–Π·Π°Ρ‚ΠΎΡ€Ρ–Π² Ρ…Ρ–ΠΌΡ–Ρ‡Π½ΠΈΡ… процСсів Π΄ΠΎ молСкулярних сСнсорів. Π£ Ρ…ΠΎΠ΄Ρ– вивчСння Ρ„ΠΎΡ€ΠΌΡ–Π»ΡŽΠ²Π°Π½Π½Ρ 5’,6’,7’,8’-Ρ‚Π΅Ρ‚Ρ€Π°Π³Ρ–Π΄Ρ€ΠΎ-1’Н-спіро[циклогСксан-1,2’-Ρ…Ρ–Π½Π°Π·ΠΎΠ»Ρ–Π½]-4’(3’Н)-ΠΎΠ½Ρƒ Π½Π°ΠΌΠΈ Π±ΡƒΠ»Π° Π²Ρ–Π΄ΠΊΡ€ΠΈΡ‚Π° Π½ΠΎΠ²Π° Π΄ΠΎΠΌΡ–Π½ΠΎ-рСакція, яка дозволяє Π²ΠΈΠΉΡ‚ΠΈ Π½Π° Ρ‚Ρ€ΠΈΡ†ΠΈΠΊΠ»Ρ–Ρ‡Π½Ρ– Π³Ρ–Π΄Ρ€ΠΎΠ²Π°Π½Ρ– Π°ΠΊΡ€ΠΈΠ΄ΠΈΠ½ΠΎΠ²Ρ– систСми. Показано, Ρ‰ΠΎ Π½Π΅Π·Π²Π°ΠΆΠ°ΡŽΡ‡ΠΈ Π½Π° Π·Π½ΠΈΠΆΠ΅Π½Ρƒ Π΅Π»Π΅ΠΊΡ‚Ρ€ΠΎΡ„Ρ–Π»ΡŒΠ½Ρ–ΡΡ‚ΡŒ Π°Π»ΡŒΠ΄Π΅Π³Ρ–Π΄Π½ΠΈΡ… Π³Ρ€ΡƒΠΏ Ρƒ 4,5-Π΄ΠΈΡ„ΠΎΡ€ΠΌΡ–Π»-2,3,6,7,8,10-гСксагідроакридину-8Π°(1Н)-ΠΊΠ°Ρ€Π±ΠΎΠ½Ρ–Ρ‚Ρ€ΠΈΠ»Ρ–, Π²Ρ–Π½ Ρ€Π΅Π°Π³ΡƒΡ” Π· Ρ€Ρ–Π·Π½ΠΈΠΌΠΈ Π°ΠΌΡ–Π½Π°ΠΌΠΈ Ρƒ Π±Π΅Π½Π·ΠΎΠ»Ρ– Π· Π°Π·Π΅ΠΎΡ‚Ρ€ΠΎΠΏΠ½ΠΎΡŽ Π²Ρ–Π΄Π³ΠΎΠ½ΠΊΠΎΡŽ Π²ΠΎΠ΄ΠΈ Π· використанням Π² якості ΠΊΠ°Ρ‚Π°Π»Ρ–Π·Π°Ρ‚ΠΎΡ€Π° p-TsOH, Π° Ρ‚Π°ΠΊΠΎΠΆ Π· солянокислим гідроксиламіном Ρƒ i-PrOH. ΠžΡ‚Ρ€ΠΈΠΌΠ°Π½Ρ– основи Π¨ΠΈΡ„Ρ„Π° Ρ‚Π° оксим ΡΡ‚Π°Π½ΠΎΠ²Π»ΡΡ‚ΡŒ ΠΏΠΎΡ‚Π΅Π½Ρ†Ρ–ΠΉΠ½ΠΈΠΉ інтСрСс Ρƒ якості Π»Ρ–Π³Π°Π½Π΄Ρ–Π² для утворСння Ρ…Π΅Π»Π°Ρ‚Π½ΠΈΡ… комплСксів. Π£ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ– Ρ€Π΅Π°ΠΊΡ†Ρ–Ρ— Π΄Ρ–Π°Π»ΡŒΠ΄Π΅Π³Ρ–Π΄Ρƒ Π· N2H4Γ—H2O Π·Π°ΠΌΡ–ΡΡ‚ΡŒ ΠΎΡ‡Ρ–ΠΊΡƒΠ²Π°Π½ΠΎΠ³ΠΎ Π³Ρ–Π΄Ρ€Π°Π·ΠΎΠ½Ρƒ ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΎ ΠΌΠ°ΠΊΡ€ΠΎΡ†ΠΈΠΊΠ»Ρ–Ρ‡Π½Ρƒ сполуку – ΠΏΠΎΡ…Ρ–Π΄Π½Ρƒ гСксаазациклооктадСцину. Π‘ΡƒΠ΄ΠΎΠ²Π° всіх ΠΎΡ‚Ρ€ΠΈΠΌΠ°Π½ΠΈΡ… сполук ΠΏΡ–Π΄Ρ‚Π²Π΅Ρ€Π΄ΠΆΠ΅Π½Π° Π΄Π°Π½ΠΈΠΌΠΈ ЯМР 1Н-спСктроскопії, мас-спСктромСтрії Ρ– Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π½ΠΎΠ³ΠΎ Π°Π½Π°Π»Ρ–Π·Ρƒ. ΠŸΠΎΠΏΠ΅Ρ€Π΅Π΄Π½Ρ– дослідТСння продСмонстрували, Ρ‰ΠΎ Π°Π·ΠΎΠΌΠ΅Ρ‚ΠΈΠ½ΠΈ – 4,5-Ρ„Π΅Π½Ρ–Π»(циклогСксил)Ρ–ΠΌΡ–Π½ΠΎΠΌΠ΅Ρ‚ΠΈΠ»-2, 3,6,7,8,10-гСксагідроакридин-8Π°(1Н)-ΠΊΠ°Ρ€Π±ΠΎΠ½Ρ–Ρ‚Ρ€ΠΈΠ»Ρƒ ΡƒΡ‚Π²ΠΎΡ€ΡŽΡŽΡ‚ΡŒ комплСксні сполуки Π· Ρ–ΠΎΠ½Π°ΠΌΠΈ Π½Ρ–ΠΊΠ΅Π»ΡŽ Ρ‚Π° ΠΌΡ–Π΄Ρ–

    Classical model of elementary particle with Bertotti-Robinson core and extremal black holes

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    We discuss the question, whether the Reissner-Nordstr\"{o}m RN) metric can be glued to another solutions of Einstein-Maxwell equations in such a way that (i) the singularity at r=0 typical of the RN metric is removed (ii), matching is smooth. Such a construction could be viewed as a classical model of an elementary particle balanced by its own forces without support by an external agent. One choice is the Minkowski interior that goes back to the old Vilenkin and Fomin's idea who claimed that in this case the bare delta-like stresses at the horizon vanish if the RN metric is extremal. However, the relevant entity here is the integral of these stresses over the proper distance which is infinite in the extremal case. As a result of the competition of these two factors, the Lanczos tensor does not vanish and the extremal RN cannot be glued to the Minkowski metric smoothly, so the elementary-particle model as a ball empty inside fails. We examine the alternative possibility for the extremal RN metric - gluing to the Bertotti-Robinson (BR) metric. For a surface placed outside the horizon there always exist bare stresses but their amplitude goes to zero as the radius of the shell approaches that of the horizon. This limit realizes the Wheeler idea of "mass without mass" and "charge without charge". We generalize the model to the extremal Kerr-Newman metric glued to the rotating analog of the BR metric.Comment: 23 pages. Misprints correcte

    3D-4D Interlinkage Of qqq Wave Functions Under 3D Support For Pairwise Bethe-Salpeter Kernels

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    Using the method of Green's functions within a Bethe-Salpeter framework characterized by a pairwise qq interaction with a Lorentz-covariant 3D support to its kernel, the 4D BS wave function for a system of 3 identical relativistic spinless quarks is reconstructed from the corresponding 3D form which satisfies a fully connected 3D BSE. This result is a 3-body generalization of a similar 2-body result found earlier under identical conditions of a 3D support to the corresponding qq-bar BS kernel under Covariant Instaneity (CIA for short). (The generalization from spinless to fermion quarks is straightforward). To set the CIA with 3D BS kernel support ansatz in the context of contemporary approaches to the qqq baryon problem, a model scalar 4D qqq BSE with pairwise contact interactions to simulate the NJL-Faddeev equations is worked out fully, and a comparison of both vertex functions shows that the CIA vertex reduces exactly to the NJL form in the limit of zero spatial range. This consistency check on the CIA vertex function is part of a fuller accounting for its mathematical structure whose physical motivation is traceable to the role of `spectroscopy' as an integral part of the dynamics.Comment: 20 pages, Latex, submitted via the account of K.-C. Yan
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