5,594 research outputs found

    Nuclear effects in positive pion electroproduction on the deuteron near threshold

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    Positive pion electroproduction from the deuteron near threshold has been considered within an approach based on the unitary transformation method. The gauge independence of the treatment is provided by using an explicitly gauge independent expression for the reaction amplitude. The results of calculations for kinematics of the experiments on forward-angle π+\pi^+ meson electroproduction accomplished at Saclay and Jefferson Laboratory are discussed and compared with those given by the impulse approximation. It is shown that the observed behaviour of the cross sections is in accordance with the calculations based on the pion-nucleon dynamics. In particular, the pion production rate suppression in the 2H(e,eπ+)nn^2H(e,e'\pi^+)nn reaction compared to that for the 1H(e,eπ+)n^1H(e,e'\pi^+)n one can be due to such ``nuclear medium'' effects as nucleon motion and binding along with Pauli blocking in the final nnnn state.Comment: 15 pages, 8 figure

    Compton Scattering from the Deuteron and Extracted Neutron Polarizabilities

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    Differential cross sections for Compton scattering from the deuteron were measured at MAX-lab for incident photon energies of 55 MeV and 66 MeV at nominal laboratory angles of 4545^\circ, 125125^\circ, and 135135^\circ. Tagged photons were scattered from liquid deuterium and detected in three NaI spectrometers. By comparing the data with theoretical calculations in the framework of a one-boson-exchange potential model, the sum and difference of the isospin-averaged nucleon polarizabilities, αN+βN=17.4±3.7\alpha_N + \beta_N = 17.4 \pm 3.7 and αNβN=6.4±2.4\alpha_N - \beta_N = 6.4 \pm 2.4 (in units of 10410^{-4} fm3^3), have been determined. By combining the latter with the global-averaged value for αpβp\alpha_p - \beta_p and using the predictions of the Baldin sum rule for the sum of the nucleon polarizabilities, we have obtained values for the neutron electric and magnetic polarizabilities of αn=8.8±2.4\alpha_n= 8.8 \pm 2.4(total) ±3.0\pm 3.0(model) and βn=6.52.4\beta_n = 6.5 \mp 2.4(total) 3.0\mp 3.0(model), respectively.Comment: 4 pages, 2 figures, revtex. The text is substantially revised. The cross sections are slightly different due to improvements in the analysi

    Neutron polarizabilities investigated by quasi-free Compton scattering from the deuteron

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    Measuring Compton scattered photons and recoil neutrons in coincidence, quasi-free Compton scattering by the neutron has been investigated at MAMI (Mainz) at thetaγlab=136otheta^{lab}_\gamma=136^o in an energy range from 200 to 400 MeV. From the data a polarizability difference of αnβn=9.8±3.6(stat)1.1+2.1(syst)±2.2(model)\alpha_n - \beta_n = 9.8 \pm 3.6(stat)^{+2.1}_{-1.1}(syst)\pm 2.2(model) in units of 104fm310^{-4}fm^3 has been determined. In combination with the polarizability sum αn+βn=15.2±0.5\alpha_n+\beta_n= 15.2\pm 0.5 deduced from photo absorption data, the neutron electric and magnetic polarizabilities, αn=12.5±1.8(stat)0.6+1.1(syst)±1.1(model)\alpha_n=12.5\pm 1.8(stat)^{+1.1}_{-0.6}(syst)\pm 1.1(model) and βn=2.71.8(stat)1.1+0.6(syst)1.1(model)\beta_n = 2.7\mp 1.8(stat)^{+0.6}_{-1.1}(syst)\mp 1.1(model), are obtained

    Comment on ``Evidence for Narrow Baryon Resonances in Inelastic pp Scattering''

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    Compton scattering data are sensitive to the existence of low-mass resonances reported by Tatischeff et al. We show that such states, with their reported properties, are excluded by previous Compton scattering experiments.Comment: One page, submitted to PR

    Neurohumoral markers that predict the efficiency of pharmacologic therapy of depressive disorders

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    We present a comprehensive clinical and biological study of 46 patients with depressive disorder (F32-F33: depressive episode and recurrent depressive disorder) during pharmacotherapy. Neurohumoral factors (cortisol, brain-derived neurotrophic factor, serotonin, DHEA and its sulfated form) were determined in serum by ELISA. The severity of the current depressive episode was evaluated using the 17-point Hamilton Depression Rating Scale (HDRS-17); the pharmacotherapy efficacy was evaluated using the scale of the Clinical Global Impression (CGI Scale). We showed that before prescription of pharmacotherapy peripheral blood neurohumoral markers that characterize the state of stress-realizing and stress-limiting systems of the body may be considered as biological predictors of the effective pharmacotherapy of a current depressive episode and used as additional paraclinical examination methods. At higher concentrations of cortisol and serotonin associated with a decrease in the content of neurosteroid dehydroepiandrosterone, the high efficiency of the pharmacotherapy of depressive episode is predicted

    An Analysis of the Chemical Composition of the Atmosphere of Venus on an AMS of the Venera-12 Using a Gas Chromatograph

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    Eight analyses of the atmosphere of Venus were made beginning at an altitude of 42 km right down to the surface of the planet. The following were detected in the atmosphere of Venus: nitrogen in concentrations of 2.5 plus or minus 0.5 volumetric %, argon ir concentrations (4 plus or minus 2) x 10 to the minus 3 power volumetric %, CO--(2.8 plus or minus 1.4) x 10 to the minus 3 power volumetric % and SO2 in concentrations (1.3 plus or minus 0.6) x 10 to the minus 2 power volumetric %. The upper limits were estimated for the content of oxygen and water equal to 2 x 10 to the minus 3 power and 10 to the minus 2 power volumetric %, respectively

    Quasi-free Compton Scattering from the Deuteron and Nucleon Polarizabilities

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    Cross sections for quasi-free Compton scattering from the deuteron were measured for incident energies of 236--260 MeV at the laboratory angle -135 degrees. The recoil nucleons were detected in a liquid-scintillator array situated at 20 degrees. The measured differential cross sections were used, with the calculations of Levchuk et al., to determine the polarizabilities of the bound nucleons. For the bound proton, the extracted values were consistent with the accepted value for the free proton. Combining our results for the bound neutron with those from Rose et al., we obtain one-sigma constraints of alpha_n = 7.6-14.0 and beta_n = 1.2-7.6.Comment: 4 pages, 3 figures, accepted in PR

    ВИКОРИСТАННЯ ТЕХНОЛОГІЙ ІНТЕРАКТИВНОГО НАВЧАННЯ У СТУДЕНТІВ МЕДИЧНОГО УЧИЛИЩА НА ЗАНЯТТЯХ ІЗ ОТОРИНОЛАРИНГОЛОГИ

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    The article adduces the basic tasks, options and methods of the interactive education on the otorhinolaryngology classes. This method promotes activity development, creativity, independence and critical thinking in students of medical colleges. The usage of interactive education technologies provides the mastering by medical students the modern models of professional activity, which is very close to the real clinical situations.У статті відображено основні завдання, варіанти та методи інтерактивного навчання студентів на заняттях із оториноларингології. Це сприяє розвитку активності, творчості, самостійності та критичного мислення у студентів медичних училищ. Використання технологій інтерактивного навчання забезпечує опанування студентами-медиками сучасних моделей професійної діяльності, максимально наближених до реальних клінічних ситуацій

    Dirac-Foldy term and the electromagnetic polarizability of the neutron

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    We reconsider the Dirac-Foldy contribution μ2/m\mu^2/m to the neutron electric polarizability. Using a Dirac equation approach to neutron-nucleus scattering, we review the definitions of Compton continuum (αˉ\bar{\alpha}), classical static (αEn\alpha^n_E), and Schr\"{o}dinger (αSch\alpha_{Sch}) polarizabilities and discuss in some detail their relationship. The latter αSch\alpha_{Sch} is the value of the neutron electric polarizability as obtained from an analysis using the Schr\"{o}dinger equation. We find in particular αSch=αˉμ2/m\alpha_{Sch} = \bar{\alpha} - \mu^2/m , where μ\mu is the magnitude of the magnetic moment of a neutron of mass mm. However, we argue that the static polarizability αEn\alpha^n_E is correctly defined in the rest frame of the particle, leading to the conclusion that twice the Dirac-Foldy contribution should be added to αSch\alpha_{Sch} to obtain the static polarizability αEn\alpha^n_E.Comment: 11 pages, RevTeX, to appear in Physical Review
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