99 research outputs found

    Measurement of J/psi to eta_c gamma at KEDR

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    We present a study of the inclusive photon spectra from 5.9 million J/psi decays collected with the KEDR detector at the VEPP-4M e+e- collider. We measure the branching fraction of radiative decay J/psi to eta_c gamma, eta_c width and mass. Our preliminary results are: M(eta_c) = 2979.4+-1.5+-1.9 MeV, G(eta_c) = 27.8+-5.1+-3.3 MeV, B(J/psi to eta_c gamma) = (2.34+-0.15+-0.40)%.Comment: To be published in Proceedings of the PhiPsi09, Oct. 13-16, 2009, Beijing, Chin

    Measurement of J/ψ→γηcJ/\psi\to\gamma\eta_{\rm c} decay rate and ηc\eta_{\rm c} parameters at KEDR

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    Using the inclusive photon spectrum based on a data sample collected at the J/ψJ/\psi peak with the KEDR detector at the VEPP-4M e+e−e^+e^- collider, we measured the rate of the radiative decay J/ψ→γηcJ/\psi\to\gamma\eta_{\rm c} as well as ηc\eta_{\rm c} mass and width. Taking into account an asymmetric photon lineshape we obtained Γγηc0=2.98±0.18∣−0.33+0.15\Gamma^0_{\gamma\eta_{\rm c}}=2.98\pm0.18 \phantom{|}^{+0.15}_{-0.33} keV, Mηc=2983.5±1.4∣−3.6+1.6M_{\eta_{\rm c}} = 2983.5 \pm 1.4 \phantom{|}^{+1.6}_{-3.6} MeV/c2c^2, Γηc=27.2±3.1∣−2.6+5.4\Gamma_{\eta_{\rm c}} = 27.2 \pm 3.1 \phantom{|}^{+5.4}_{-2.6} MeV.Comment: 6 pages, 3 figure

    Measurement of B(J/psi->eta_c gamma) at KEDR

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    We present a study of the inclusive photon spectrum from 6.3 million J/psi decays collected with the KEDR detector at the VEPP-4M e+e- collider. We measure the branching fraction of the radiative decay J/psi -> eta_c gamma, eta_c width and mass. Taking into account an asymmetric photon line shape we obtain: M(eta_c) = (2978.1 +- 1.4 +- 2.0) MeV/c^2, Gamma(eta_c) = (43.5 +- 5.4 +- 15.8) MeV, B(J/psi->eta_c gamma) = (2.59 +- 0.16 +- 0.31)%$.Comment: 6 pages, 1 figure. To be published in the proceedings of the 4th International Workshop on Charm Physics (Charm2010), October 21-24, 2010, IHEP, Beijin

    Precise measurement of RudsR_{\text{uds}} and RR between 1.84 and 3.72 GeV at the KEDR detector

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    The present work continues a series of the KEDR measurements of the RR value that started in 2010 at the VEPP-4M e+e−e^+e^- collider. By combining new data with our previous results in this energy range we measured the values of RudsR_{\text{uds}} and RR at nine center-of-mass energies between 3.08 and 3.72 GeV. The total accuracy is about or better than 2.6%2.6\% at most of energy points with a systematic uncertainty of about 1.9%1.9\%. Together with the previous precise RR measurement at KEDR in the energy range 1.84-3.05 GeV, it constitutes the most detailed high-precision RR measurement near the charmonium production threshold.Comment: arXiv admin note: text overlap with arXiv:1610.02827 and substantial text overlap with arXiv:1510.0266

    Status of the Super-B factory Design

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    The SuperB international team continues to optimize the design of an electron-positron collider, which will allow the enhanced study of the origins of flavor physics. The project combines the best features of a linear collider (high single-collision luminosity) and a storage-ring collider (high repetition rate), bringing together all accelerator physics aspects to make a very high luminosity of 1036^{36} cm−2^{-2} sec−1^{-1}. This asymmetric-energy collider with a polarized electron beam will produce hundreds of millions of B-mesons at the Υ\Upsilon(4S) resonance. The present design is based on extremely low emittance beams colliding at a large Piwinski angle to allow very low βy⋆\beta_y^\star without the need for ultra short bunches. Use of crab-waist sextupoles will enhance the luminosity, suppressing dangerous resonances and allowing for a higher beam-beam parameter. The project has flexible beam parameters, improved dynamic aperture, and spin-rotators in the Low Energy Ring for longitudinal polarization of the electron beam at the Interaction Point. Optimized for best colliding-beam performance, the facility may also provide high-brightness photon beams for synchrotron radiation applications

    EPIDEMIOLOGICAL AND EPIZOOTIOLOGICAL ANALYSIS OF THE SITUATION ON TULAREMIA IN THE RUSSIAN FEDERATION IN 2016 AND FORECAST FOR 2017

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    123 cases of human infection with Francisella tularensis were registered in the territory of the Russian Federation in 2016. 90 % of the total number was reported by three Federal Districts: North-Western, Siberian, and Central ones. Epizootic manifestations of varying intensity were detected in 56 regions. A considerable number of tularemia cases were observed in the Republic of Karelia, Nenets Autonomous District, Omsk and Ryazan Regions, and in Saint-Petersburg. Conspicuous are some recent peculiarities of tularemia manifestations: non-specificity of clinical symptoms, especially at early stages of the disease, their increasing variability against the background of mixed infections with tularemia and other natural-focal infections agents. The most expressed symptoms are fever and lymphatic adenitis; the patients are diagnosed with tularemia during initial days of the sought treatment in 40-45 % of the cases. Based on the data on morbidity rates in humans, epizootiological condition of natural tularemia foci, the numbers of isolated cultures and incidence of the vectors and carriers of the agent, as well as taking into consideration the scope of preventive vaccination in the regions, identified were the territories in which epidemic complication are most likely to occur in 2017

    Small-scale solar magnetic fields

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    As we resolve ever smaller structures in the solar atmosphere, it has become clear that magnetism is an important component of those small structures. Small-scale magnetism holds the key to many poorly understood facets of solar magnetism on all scales, such as the existence of a local dynamo, chromospheric heating, and flux emergence, to name a few. Here, we review our knowledge of small-scale photospheric fields, with particular emphasis on quiet-sun field, and discuss the implications of several results obtained recently using new instruments, as well as future prospects in this field of research.Comment: 43 pages, 18 figure

    Measurement of Γee(J/ψ)\Gamma_{ee}(J/\psi) with KEDR detector

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    The product of the electronic width of the J/ψJ/\psi meson and the branching fractions of its decay to hadrons and electrons has been measured using the KEDR detector at the VEPP-4M e+e−e^+e^- collider. The obtained values are: Γee(J/ψ)=5.550±0.056±0.089 keV,\Gamma_{ee}(J/\psi) = 5.550 \pm 0.056 \pm 0.089 \, \text{keV}, Γee(J/ψ)⋅Bhadrons(J/ψ)=4.884±0.048±0.078 keV,\Gamma_{ee}(J/\psi) \cdot \mathcal{B}_\text{hadrons}(J/\psi) = 4.884 \pm 0.048 \pm 0.078 \, \text{keV}, Γee(J/ψ)⋅Bee(J/ψ)=0.3331±0.0066±0.0040 keV.\Gamma_{ee}(J/\psi) \cdot \mathcal{B}_{ee}(J/\psi) = 0.3331 \pm 0.0066 \pm 0.0040 \, \text{keV}. The uncertainties shown are statistical and systematic, respectively. Using the result presented and the world-average value of the electronic branching fraction, one obtains the total width of the J/ψJ/\psi meson: Γ=92.94±1.83 keV.\Gamma = 92.94 \pm 1.83 \, \text{keV}. These results are consistent with the previous experiments.Comment: 19 pages, 13 figure
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