Search Results - "Ruber, R"

Double-pionic fusion of nuclear systems and the "ABC" effect: approaching a puzzle by exclusive and kinematically complete measurements by Bashkanov, M, Bargholtz, C, Berłowski, M, Bogoslawsky, D, Calén, H, Clement, H, Demiroers, L, Doroshkevich, E, Duniec, D, Ekström, C, Fransson, K, Geren, L, Gustafsson, L, Höistad, B, Ivanov, G, Jacewicz, M, Jiganov, E, Johansson, T, Khakimova, O, Keleta, S, Koch, I, Kren, F, Kullander, S, Kupść, A, Lindberg, K, Marciniewski, P, Meier, R, Morosov, B, Pauly, C, Pettersson, H, Petukhov, Y, Povtorejko, A, Pricking, A, Ruber, R J M Y, Schönning, K, Scobel, W, Shwartz, B, Skorodko, T, Sopov, V, Stepaniak, J, Tegner, P-E, Thörngren-Engblom, P, Tikhomirov, V, Turowiecki, A, Wagner, G J, Wolke, M, Zabierowski, J, Zartova, I, Złomanczuk, J

“…The ABC effect-a puzzling low-mass enhancement in the pipi invariant mass spectrum, first observed by Abashian, Booth, and Crowe-is well known from inclusive…”
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Design of a Canted-Cosine-Theta Orbit Corrector for the High Luminosity LHC by Pepitone, K., Kirby, G., Ruber, R., Ahl, A., Canale, M., Dugic, I., Gentini, L., Johansson, M., Karlsson, G., Kovacikova, J., Lindstrom, J., Olsson, A., Olvegard, M.

“…The High Luminosity LHC requires dipole orbit correctors grouped in double aperture magnet assemblies. They provide a field of 3.1 T at 100 A in an aperture of…”
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Modeling Results of the Quench Behavior of a Nb-Ti Canted-Cosine-Theta Corrector Magnet for LHC by Bagni, T., Ahl, A., Almstrom, M., Canale, M., Dugic, I., Emilsson, F., Gentini, L., Haralanova, V., Johansson, M., Karlsson, G., Kennborn, B., Kirby, G., Kovacikova, J., Lindstrom, J., Pepitone, K., Pettersson, M., Olsson, A., Ruber, R., Santiago Kern, Rocio, Svanberg, C., Olvegard, M.

“…A newly designed superconducting magnet of the Canted-Cosine-Theta (CCT) type was developed as a result of a collaboration between Swedish universities…”
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Design and fabrication of a canted-cosine-theta double aperture orbit corrector dipole for the LHC by Pepitone, K., Kirby, G., Olvegard, M., Ahl, A., Almstrom, M., Dugic, I., Emilsson, F., Haralanova, V., Johansson, M., Karlsson, G., Kennborn, B., Kovacikova, J., Lindstrom, J., Olsson, A., Pettersson, M., Ruber, R.

“…A prototype CCT dipole magnet developed by a collaboration between Swedish universities, Swedish industry and CERN will be tested at Uppsala University. This…”
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Spectrometers for RF breakdown studies for CLIC by Jacewicz, M., Ziemann, V., Ekelöf, T., Dubrovskiy, A., Ruber, R.

“…An e+e− collider of several TeV energy will be needed for the precision studies of any new physics discovered at the LHC collider at CERN. One promising…”
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Two-pion production in proton–proton collisions — experimental total cross sections and their isospin decomposition by Skorodko, T., Bashkanov, M., Bogoslawsky, D., Calén, H., Clement, H., Doroshkevich, E., Demiroers, L., Ekström, C., Fransson, K., Gustafsson, L., Höistad, B., Ivanov, G., Jacewicz, M., Jiganov, E., Johansson, T., Khakimova, O., Keleta, S., Koch, I., Kren, F., Kullander, S., Kupść, A., Marciniewski, P., Meier, R., Morosov, B., Pauly, C., Petrén, H., Petukhov, Y., Povtorejko, A., Ruber, R.J.M.Y., Schönning, K., Scobel, W., Shwartz, B., Stepaniak, J., Thörngren-Engblom, P., Tikhomirov, V., Wagner, G.J., Wolke, M., Yamamoto, A., Zabierowski, J., Zlomanczuk, J.

“…The two-pion production in pp-collisions has been investigated at CELSIUS in exclusive measurements from threshold up to Tp=1.36 GeV. Total and differential…”
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Measuring the full transverse beam matrix using a single octupole by Ögren, J., Ruber, R., Ziemann, V., Farabolini, W.

“…We propose a method to fully determine the transverse beam matrix using a simple setup consisting of two steering magnets, an octupole field and a screen. This…”
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An 8-1 Single-Stage 10-kW Planar Gysel Power Combiner at 352 MHz by Jobs, M., Dancila, D., Eriksson, J., Ruber, R.

“…A compact single-stage 8-1 Gysel Combiner in planar technology for operation with 352-MHz pulses with peak output power of 10 kW has been designed,…”
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The WASA detector facility at CELSIUS by Bargholtz, Chr, Bashkanov, M., Berłowski, M., Bondar, A., Bogoslawsky, D., Brodowski, W., Brudvik, J., Calén, H., Capellaro, F., Chilingarov, A., Clement, H., Comfort, J., Demirörs, L., Ekström, C., Fransson, K., Fridén, C.-J., Gerén, L., Gornov, M., Grebenev, V., Greiff, J., Gurov, Y., Gustafsson, L., Höistad, B., Ivanov, G., Jacewicz, M., Jiganov, E., Johansson, A., Johansson, T., Keleta, S., Khakimova, O., Khoukaz, A., Kilian, K., Kimura, N., Koch, I., Kolachev, G., Kren, F., Kullander, S., Kupść, A., Kuzmin, A., Kuznetsov, A., Lindberg, K., Marciniewski, P., Meier, R., Messner, O., Morosov, B., Nawrot, A., Nefkens, B.M.K., Norman, G., Oelert, W., Pauly, C., Pettersson, H., Pivovarov, A., Pätzold, J., Petukhov, Y., Povtorejko, A., Reistad, D., Ruber, R.J.M.Y., Sandukovsky, S., Schönning, K., Scobel, W., Sefzick, T., Shafigullin, R., Shwartz, B., Sidorov, V., Skorodko, T., Sopov, V., Starostin, A., Stepaniak, J., Sukhanov, A., Sukhanov, A., Tchernyshev, V., Tegnér, P.-E., Thörngren Engblom, P., Tikhomirov, V., Toki, H., Turowiecki, A., Wagner, G.J., Wiedner, U., Wilhelmi, Z., Wolke, M., Yamamoto, A., Yamaoka, H., Zabierowski, J., Zartova, I., Złomańczuk, J.

“…The WASA 4 π multidetector system, aimed at investigating light meson production in light ion collisions and η meson rare decays at the CELSIUS storage ring in…”
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The European Spallation Source by Lindroos, M., Bousson, S., Calaga, R., Danared, H., Devanz, G., Duperrier, R., Eguia, J., Eshraqi, M., Gammino, S., Hahn, H., Jansson, A., Oyon, C., Pape-Møller, S., Peggs, S., Ponton, A., Rathsman, K., Ruber, R., Satogata, T., Trahern, G.

“…In 2003 the joint European effort to design a European Spallation Source (ESS) resulted in a set of reports, and in May 2009 Lund was agreed to be the ESS…”
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The CTF3 Two-beam Test Stand by Ruber, R., Ziemann, V., Ekelöf, T., Palaia, A., Farabolini, W., Corsini, R.

“…The Two-beam Test Stand (TBTS) has been constructed and operated at the CLIC test facility CTF3 at CERN. The TBTS comprises two parallel and independent…”
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Erratum: Effects of rf breakdown on the beam in the Compact Linear Collider prototype accelerator structure [Phys. Rev. ST Accel. Beams 16 , 081004 (2013)] by Palaia, A., Jacewicz, M., Ruber, R., Ziemann, V., Farabolini, W.

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Effects of rf breakdown on the beam in the Compact Linear Collider prototype accelerator structure by Palaia, A., Jacewicz, M., Ruber, R., Ziemann, V., Farabolini, W.

“…Understanding the effects of rf breakdown in high-gradient accelerator structures on the acceleratedbeam is an extremely relevant aspect in the development of…”
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The Opportunity Offered by the ESSnuSB Project to Exploit the Larger Leptonic CP Violation Signal at the Second Oscillation Maximum and the Requirements of This Project on the ESS Accelerator Complex by Wildner, E., Baussan, E., Blennow, M., Bogomilov, M., Burgman, A., Bouquerel, E., Carlile, C., Cederkäll, J., Christiansen, P., Cupial, P., Danared, H., Dracos, M., Ekelöf, T., Eshraqi, M., Hall-Wilton, R., Koutchouk, J.-P., Lindroos, M., Martini, M., Matev, R., McGinnis, D., Miyamoto, R., Ohlsson, T., Öhman, H., Olvegård, M., Ruber, R., Schönauer, H., Tang, J. Y., Tsenov, R., Vankova-Kirilova, G., Vassilopoulos, N.

“…The European Spallation Source (ESS), currently under construction in Lund, Sweden, is a research center that will provide, by 2023, the world’s most powerful…”
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X -band rf power production and deceleration in the two-beam test stand of the Compact Linear Collider test facility by Adli, E., Ruber, R., Ziemann, V., Corsini, R., Dubrovskiy, A., Syratchev, I.

“…We discuss X-band rf power production and deceleration in the two-beam test stand of the CLIC test facility at CERN. The rf power is extracted from an electron…”
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Arrival time measurements of ions accompanying RF breakdown by Johnson, M., Ruber, R., Ziemann, V., Braun, H.

“…Radio-frequency structures for future normal-conducting linear accelerators are limited in accelerating gradient levels by RF breakdown in the structures due…”
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The ATLAS central solenoid by Yamamoto, A., Makida, Y., Ruber, R., Doi, Y., Haruyama, T., Haug, F., ten Kate, H., Kawai, M., Kondo, T., Kondo, Y., Metselaar, J., Mizumaki, S., Olesen, G., Pavlov, O., Ravat, S., Sbrissa, E., Tanaka, K., Taylor, T., Yamaoka, H.

“…The ATLAS detector at the CERN LHC is equipped with a superconducting magnet system consisting of three large toroids and a solenoid. The 2.3 m diameter, 5.3 m…”
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Evolution of superconducting detector magnets by Ruber, R.J.M.Y., Yamamoto, A.

“…The increase of energy in colliding particle beams as well as the advances in particle detector technology during the last three decades have led to an…”
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Measurement of the η→π+π−e+e− decay branching ratio by Bargholtz, Chr, Bashkanov, M., Bogoslawsky, D., Calén, H., Cappellaro, F., Clement, H., Demirörs, L., Ekström, C., Fransson, K., Gerén, L., Gustafsson, L., Höistad, B., Ivanov, G., Jacewicz, M., Jiganov, E., Johansson, T., Keleta, S., Koch, I., Kullander, S., Kupść, A., Kuznetsov, A., Laukhin, I.V., Lindberg, K., Marciniewski, P., Meier, R., Morosov, B., Oelert, W., Pauly, C., Pettersson, H., Petukhov, Y., Povtorejko, A., Ruber, R.J.M.Y., Schönning, K., Scobel, W., Shafigullin, R., Shwartz, B., Skorodko, T., Sopov, V., Stepaniak, J., Tchernyshev, V., Tegnér, P.-E., Thörngren Engblom, P., Tikhomirov, V., Turowiecki, A., Wagner, G.J., Wolke, M., Yamamoto, A., Zabierowski, J., Zartova, I., Złomańczuk, J.

“…The reaction pd→He3η at threshold was used to provide a clean source of η mesons for decay studies with the WASA detector at CELSIUS. The branching ratio of…”
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Two-pion production in proton–proton collisions near threshold by Johanson, J., Bilger, R., Brodowski, W., Calén, H., Clement, H., Ekström, C., Fransson, K., Greiff, J., Gustafsson, L., Häggström, S., Höistad, B., Johansson, A., Johansson, T., Khoukaz, A., Koch, I., Kullander, S., Kupsc, A., Marciniewski, P., Morosov, B., Oelert, W., Povtorejko, A., Ruber, R., Scobel, W., Sefzick, T., Shwartz, B., Stepaniak, J., Sukhanov, A., Wagner, G.J., Zabierowski, J., Zlomańczuk, J.

“…Two-pion production reactions in proton–proton collisions have been studied using the PROMICE/ WASA detector and an internal cluster gas-jet target at the…”
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