66 research outputs found

    Measurement of J/Ïˆâ†’ÎłÎ·cJ/\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/Ïˆâ†’ÎłÎ·cJ/\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 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 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

    Building the impedance model of a real machine

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    A reliable impedance model of a particle accelerator can be built by combining the beam coupling impedances of all the components. This is a necessary step to be able to evaluate the machine performance limitations, identify the main contributors in case an impedance reduction is required, and study the interaction with other mechanisms such as optics nonlinearities, transverse damper, noise, space charge, electron cloud, beam-beam (in a collider). The main phases to create a realistic impedance model, and verify it experimentally, will be reviewed, highlighting the main challenges. Some examples will be presented revealing the levels of precision of machine impedance models that have been achieved

    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

    Status of VEPP-4M collider: current activity and plans

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    Presented are the results of a VEPP-4M collider operation at Budker Institute of Nuclear Physics during 2004-2005 as well as the plans for the nearest future.ĐŸŃ€Đ”ĐŽŃŃ‚Đ°ĐČĐ»Đ”ĐœŃ‹ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹, ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœĐœŃ‹Đ” ĐœĐ° ĐœĐ°ĐșĐŸĐżĐžŃ‚Đ”Đ»Đ” ВЭПП-4М Đ˜ĐœŃŃ‚ĐžŃ‚ŃƒŃ‚Đ° ĐŻĐŽĐ”Ń€ĐœĐŸĐč фОзОĐșĐž ĐžĐŒ. БуЮĐșДра, Đ·Đ° ĐżĐ”Ń€ĐžĐŸĐŽ 2004-2005 Đł., Đ° таĐșжД ĐżĐ»Đ°ĐœŃ‹ ĐœĐ° блОжаĐčшДД Đ±ŃƒĐŽŃƒŃ‰Đ”Đ”.ĐŸŃ€Đ”ĐŽŃŃ‚Đ°ĐČĐ»Đ”ĐœĐŸ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž, ĐŸŃ‚Ń€ĐžĐŒĐ°ĐœŃ– ĐœĐ° ĐœĐ°ĐșĐŸĐżĐžŃ‡ŃƒĐČачі ВЕПП-4М Đ†ĐœŃŃ‚ĐžŃ‚ŃƒŃ‚Ńƒ ĐŻĐŽĐ”Ń€ĐœĐŸŃ— Ń„Ń–Đ·ĐžĐșĐž Ń–ĐŒ. БуЮĐșДра, Đ·Đ° ĐżĐ”Ń€Ń–ĐŸĐŽ 2004-2005 р., Đ° таĐșĐŸĐ¶ ĐżĐ»Đ°ĐœĐž ĐœĐ° ĐœĐ°ĐčблОжчД ĐŒĐ°ĐčĐ±ŃƒŃ‚Đœ

    THE DOUBLE-DOUBLE BEND ACHROMAT (DDBA) LATTICE MODIFICATION FOR THE DIAMOND STORAGE RING

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    Abstract We present an overview of the status of the DDBA project, the various accelerator physics and engineering studies that have been carried out, and plans for the implementation of one or two DDBA cells in Diamond

    FCC-ee: The Lepton Collider – Future Circular Collider Conceptual Design Report Volume 2

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    HE-LHC: The High-Energy Large Hadron Collider – Future Circular Collider Conceptual Design Report Volume 4

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    In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the third volume of the FCC Conceptual Design Report, devoted to the hadron collider FCC-hh. It summarizes the FCC-hh physics discovery opportunities, presents the FCC-hh accelerator design, performance reach, and staged operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. Its unprecedented centre-of-mass collision energy will make the FCC-hh a unique instrument to explore physics beyond the Standard Model, offering great direct sensitivity to new physics and discoveries
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