807 research outputs found

    A note on N=4 supersymmetric mechanics on K\"ahler manifolds

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    The geometric models of N=4 supersymmetric mechanics with (2d.2d)_{\DC}-dimensional phase space are proposed, which can be viewed as one-dimensional counterparts of two-dimensional N=2 supersymmetric sigma-models by Alvarez-Gaum\'e and Freedman. The related construction of supersymmetric mechanics whose phase space is a K\"ahler supermanifold is considered. Also, its relation with antisymplectic geometry is discussed.Comment: 4 pages, revte

    Increasing the efficiency of heating systems through the use of direct contact heat exchange

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    You should leave 8 mm of space above the abstract and 10 mm after the abstract. The heading Abstract should be typed in bold 9-point Arial. The body of the abstract should be typed in normal 9-point Times in a single paragraph, immediately following the heading. The text should be set to 1 line spacing. The abstract should be centred across the page, indented 17 mm from the left and right page margins and justified. It should not normally exceed 200 words

    ΠŸΠ΅Ρ€Π²Π°Ρ краСвая Π·Π°Π΄Π°Ρ‡Π° для уравнСния тСплопроводности с Π½Π°Π³Ρ€ΡƒΠ·ΠΊΠΎΠΉ Π΄Ρ€ΠΎΠ±Π½ΠΎΠ³ΠΎ порядка. II

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    Π’ ΡΡ‚Π°Ρ‚ΡŒΠ΅ рассмотрСна пСрвая краСвая Π·Π°Π΄Π°Ρ‡Π° для Π½Π°Π³Ρ€ΡƒΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ уравнСния тСплопроводности Π² Ρ‡Π΅Ρ‚Π²Π΅Ρ€Ρ‚ΠΈ плоскости. НагруТСнноС слагаСмоС - слСд ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½ΠΎΠΉ Π΄Ρ€ΠΎΠ±Π½ΠΎΠ³ΠΎ порядка Π½Π° ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±Ρ€Π°Π·ΠΈΠΈ x=t. РСшСниС Π·Π°Π΄Π°Ρ‡ΠΈ сводится ΠΊ исслСдованию особого ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ уравнСния Π’ΠΎΠ»ΡŒΡ‚Π΅Ρ€Ρ€Π° Π²Ρ‚ΠΎΡ€ΠΎΠ³ΠΎ Ρ€ΠΎΠ΄Π° с нСсТимаСмым ядром. РСшСниС характСристичСского уравнСния ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ рСгуляризации ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ, Ρ‡Ρ‚ΠΎ особоС ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΎΠ΅ ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠ΅ Π’ΠΎΠ»ΡŒΡ‚Π΅Ρ€Ρ€Π° ΠΈΠΌΠ΅Π΅Ρ‚ нСпустой спСктр ΠΏΡ€ΠΈ 1/2≀β<1. Π”ΠΎΠΊΠ°Π·Π°Π½Π° Ρ‚Π΅ΠΎΡ€Π΅ΠΌΠ° осущСствовании Π½Π΅Ρ‚Ρ€ΠΈΠ²ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ ΠΎΠ΄Π½ΠΎΡ€ΠΎΠ΄Π½ΠΎΠΉ ΠΊΡ€Π°Π΅Π²ΠΎΠΉ Π·Π°Π΄Π°Ρ‡ΠΈ Π² Π½Π΅ΠΎΠ³Ρ€Π°Π½ΠΈΡ‡Π΅Π½Π½ΠΎΠΉ области

    On the boundary value problem for the vibration and wave processes in two-dimensional environs

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    In the article research of the third boundary value problem for the two - dimensional equation of free membrane vibrations is presented. The solution of the original differential operator is found in the form of a combination of the linearly independent system of orthonormal eigenfunctions on the given interval. Using the spectral decomposition for sufficiently smooth function, one can obtain the exact analytical representation of the deflection function for investigated problem in two - dimensional environs. The deflection function characterizes a membrane deviation from the equilibrium position

    Experimental Study of Coherent Summation of Radiation from Two Widely Aperture Pulsed

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    Emission of two high-power pulsed CO2-lasers with a transverse discharge at atmospheric pressure in the active medium and the output beam aperture 100Ρ…100 mm, united by a joint unstable telescopic reso-nator, was coherently summarized under conditions of real ground-level trackon the screen surface, which was remote from output mirror of the laser at a distance of 263 m. Output Brewster windows of laser cu-vettes were manufactured from single-crystal plates of sodium chloride which had a diameter of 300 mm. Mirrors for resonator and optical circuit were manufactured from oxygen-free copper. Active medium - a mixture of gases: CO2: N2: He in the ratio 1 : 2 : 3. Laser pulse duration is 5 microseconds. During the ex-periment, when summing on the screen 2-laser beams at the lowest possible convergence angle of rays, the interference pattern was registered. When you are citing the document, use the following link http://essuir.sumdu.edu.ua/handle/123456789/3610

    Higher Spins from Tensorial Charges and OSp(N|2n) Symmetry

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    It is shown that the quantization of a superparticle propagating in an N=1, D=4 superspace extended with tensorial coordinates results in an infinite tower of massless spin states satisfying the Vasiliev unfolded equations for free higher spin fields in flat and AdS_4 N=1 superspace. The tensorial extension of the AdS_4 superspace is proved to be a supergroup manifold OSp(1|4). The model is manifestly invariant under an OSp(N|8) (N=1,2) superconformal symmetry. As a byproduct, we find that the Cartan forms of arbitrary Sp(2n) and OSp(1|2n) groups are GL(2n) flat, i.e. they are equivalent to flat Cartan forms up to a GL(2n) rotation. This property is crucial for carrying out the quantization of the particle model on OSp(1|4) and getting the higher spin field dynamics in super AdS_4, which can be performed in a way analogous to the flat case.Comment: LaTeX, 21 page (JHEP style), misprints corrected, added comments on the relation of results of hep-th/0106149 with hep-th/9904109 and hep-th/9907113, references adde

    Photoionization in the presence of circularly polarized fundamental and odd-order harmonic fields

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    We present a study of the photoelectron spectra for the ionization process driven by counterrotating and corotating circularly polarized fundamental and odd-order harmonic fields. The main features of the spectra, such as symmetric lobed structures, are understood using simple arguments based on the strong field approximation (SFA) picture of ionization. A deviation from this picture is, most notably, the presence of the low-energy structures (LES) in the spectra. We show that the Rydberg states populated as a result of the combined absorption of the photons from the fundamental and harmonic fields are responsible for the origin of LES. Β© 2017 American Physical Society1111Nsciescopu

    On the solution of boundary value problems by the spectral element method

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    In spectral element method approximate solution of the original differential operator is found in the form of a combination of the linearly independent system of orthogonal functions on the unit interval. Using the spectral decomposition for sufficiently smooth functions, one can obtain an exponential rate of convergence of the approximate solution to the exact solution and the approximation error will decrease exponentially as n grows. In the article the application of spectral element method to the solution of the boundary value problem for the Poisson equation is presented

    Gauge Invariance and Anomalous Dimensions of a Light-Cone Wilson Loop in Light-Like Axial Gauge

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    Complete two-loop calculation of a dimensionally regularized Wilson loop with light-like segments is performed in the light-like axial gauge with the Mandelstam-Leibbrandt prescription for the gluon propagator. We find an expression which {\it exactly} coincides with the one previously obtained for the same Wilson loop in covariant Feynman gauge. The renormalization of Wilson loop is performed in the \MS-scheme using a general procedure tailored to the light-like axial gauge. We find that the renormalized Wilson loop obeys a renormalization group equation with the same anomalous dimensions as in covariant gauges. Physical implications of our result for investigation of infrared asymptotics of perturbative QCD are pointed out.Comment: 24 pages and 4 figures (included), LaTeX style, UFPD-93/TH/23, UPRF-93-366, UTF-93-29

    ΠŸΠ΅Π»ΡŒΠ²ΠΈΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ приминСния ядСрно-ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠ³ΠΎ рСзонанса ΠΏΡ€ΠΈ субклиничСских Ρ„ΠΎΡ€ΠΌΠ°Ρ… ΡƒΠ·ΠΊΠΎΠ³ΠΎ Ρ‚Π°Π·Π° ΠΈ опрСдСлСния риска Π² случаС дистоции ΠΏΡ€Π΅Ρ‡ΠΈΠΊΠΎΠ²

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    Military Medical Academy, Department of radiology, St-Petersburg, Russia, Federal Center of blood, heart and endocrinology by VA. Almazov, St-Petersburg, RussiaΠ’ΠΎ ΠΌΠ½ΠΎΠ³ΠΈΡ… странах Ρ‚ΠΎΡ‡Π½ΠΎΡΡ‚ΡŒ ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠΉ Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ² Π½Π°Ρ€ΡƒΠΆΠ½ΠΎΠ³ΠΎ Ρ‚Π°Π·Π° ΡΠΎΠΌΠ½ΠΈΡ‚Π΅Π»ΡŒΠ½Π°. Π Π°ΡΠΏΡ€ΠΎΡΡ‚Ρ€Π°Π½Π΅Π½Π½ΠΎΡΡ‚ΡŒ ΠΏΠΎΠ΄Ρ‚ΠΈΠΏΠΎΠ² субклиничСски ΡƒΠ·ΠΊΠΎΠ³ΠΎ костного Ρ‚Π°Π·Π° Π΅Ρ‰Π΅ Π±ΠΎΠ»Π΅Π΅ затрудняСт диагностику. ЦСль: ΡƒΡΡ‚Π°Π½ΠΎΠ²ΠΈΡ‚ΡŒ Π°ΠΊΡƒΡˆΠ΅Ρ€ΡΠΊΠΈΠ΅ МР ΠΏΠ΅Π»ΡŒΠ²ΠΈΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡ‡Π΅ΡΠΊΠΈΠ΅ ΠΈ фСтомСтричСскиС рСфСрСнсныС значСния ΠΏΡ€ΠΈ ΠΎΡ†Π΅Π½ΠΊΠ΅ риска дистоции ΠΏΠ»Π΅Ρ‡ΠΈΠΊΠΎΠ² ΠΏΠ»ΠΎΠ΄Π° ΠΏΠ΅Ρ€Π΅Π΄ Ρ€ΠΎΠ΄Π°ΠΌΠΈ ΠΈ ΡΡ€Π°Π²Π½ΠΈΡ‚ΡŒ МР ΠΏΠ΅Π»ΡŒΠ²ΠΈΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡŽ с Π½Π°Ρ€ΡƒΠΆΠ½Ρ‹ΠΌΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ измСрСния. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: обслСдованы 40 ΠΆΠ΅Π½Ρ‰ΠΈΠ½ с ΠΎΠ΄Π½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ Π±Π΅Ρ€Π΅ΠΌΠΎΠ½Π½ΠΎΡΡ‚ΡŒΡŽ Π² срокС 38-39 нСдСль. МР ΠΏΠ΅ΠΏΡŒΠ²ΠΈΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΠ»Π°ΡΡŒ Π½Π° Π²Ρ‹ΡΠΎΠΊΠΎΠΏΠΎΠ»ΡŒΠ½ΠΎΠΌ 1,5 Π’ MRT. ВсС субклиничСскиС Ρ‚ΠΈΠΏΡ‹ ΡƒΠ·ΠΊΠΎΠ³ΠΎ костного Ρ‚Π°Π·Π° Π±Ρ‹Π»ΠΈ Ρ€Π°Π·Π΄Π΅Π»Π΅Π½Ρ‹ Π½Π° 3 стСпСни. ΠŸΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»Π°ΡΡŒ Ρ‚Π°ΠΊΠΆΠ΅ фСтомСтрия. Риск дистоции опрСдСлялся ΠΊΠ°ΠΊ ΠΌΠΈΠ½ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΉ, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹ΠΉ ΠΈ высокий. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹: ΠΠ±ΡΠΎΠ»ΡŽΡ‚Π½ΠΎ ΡƒΠ·ΠΊΠΈΠΉ Ρ‚Π°Π· Π±Ρ‹Π» выявлСн Ρƒ 3 ΠΆΠ΅Π½Ρ‰ΠΈΠ½. Π”ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€ костного Ρ‚Π°Π·Π°, ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½Π½Ρ‹ΠΉ Π½Π° МРВ, Π±Ρ‹Π» Π½ΠΎΡ€ΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΌ Ρƒ 14 (35%) ΠΆΠ΅Π½Ρ‰ΠΈΠ½. Π”Π²Π΅Π½Π°Π΄Ρ†Π°Ρ‚ΠΈ ΠΆΠ΅Π½Ρ‰ΠΈΠ½Π°ΠΌ (30%) со 2 ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒΡŽ ΡƒΠ·ΠΊΠΎΠ³ΠΎ Ρ‚Π°Π·Π° ΠΈ/ΠΈΠ»ΠΈ ΠΊΡ€ΡƒΠΏΠ½Ρ‹ΠΌ ΠΏΠ»ΠΎΠ΄ΠΎΠΌ (>4000 Π³) ΠΏΡ€ΠΈ отсутствии Π΄Ρ€ΡƒΠ³ΠΈΡ… ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠΏΠΎΠΊΠ°Π·Π°Π½ΠΈΠΉ Π±Ρ‹Π»ΠΎ Ρ€Π΅ΠΊΠΎΠΌΠ΅Π½Π΄ΠΎΠ²Π°Π½ΠΎ Ρ€ΠΎΠ΄ΠΎΡ€Π°Π·Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ Ρ‡Π΅Ρ€Π΅Π· СстСствСнныС Ρ€ΠΎΠ΄ΠΎΠ²Ρ‹Π΅ ΠΏΡƒΡ‚ΠΈ, Π½ΠΎ 6 ΠΈΠ· Π½ΠΈΡ… Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½ΠΎ КБ. Π—Π°ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΠ΅: низкая частота выявлСния субклиничСски ΡƒΠ·ΠΊΠΎΠ³ΠΎ костного Ρ‚Π°Π·Π° ΠΏΡ€ΠΈ Π½Π°Ρ€ΡƒΠΆΠ½Ρ‹Ρ… измСрСниях ΠΌΠΎΠΆΠ΅Ρ‚ ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ΡŒ ΠΊ Π·Π°ΠΏΠΎΠ·Π΄Π°Π»ΠΎΠΉ ΠΈΠ½Ρ‚Ρ€Π°Π½Π°Ρ‚Π°Π»ΡŒΠ½ΠΎΠΉ диагностики этой ΠΏΠ°Ρ‚ΠΎΠ»ΠΎΠ³ΠΈΠΈ. МР ΠΏΠ΅Π»ΡŒΠ²ΠΈΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΡ выявляла субклиничСскоС суТСниС костного Ρ‚Π°Π·Π°. Π”ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ Π΄Π°Π½Π½Ρ‹Π΅ Ρ„Π΅Ρ‚ΠΎΠΌΠ΅Ρ‚Ρ€ΠΈΠΈ ΠΏΠΎΠΌΠΎΠ³Π»ΠΈ ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ риск дистоции ΠΏΠ»Π΅Ρ‡ΠΈΠΊΠΎΠ² ΠΏΠ΅Ρ€Π΅Π΄ Ρ€ΠΎΠ΄Π°ΠΌΠΈ
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