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Browsing by Author "Proff, S."

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Now showing 1 - 6 of 6
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    A photon tagging system for the GDH-experiment at ELSA
    (Elsevier Science Bv, 2003)
    Naumann, J.
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    Anton, G.
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    Bock, A.
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    Grabmayr, P.
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    Helbing, Krister
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    Kiel, B.
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    Menze, D.
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    Michel, Tanja Maria
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    Proff, S.
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    Sauer, M.  
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    Schumacher, M.
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    Speckner, T.
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    Weihofen, W.
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    Zeitler, G.
    This paper describes the set-up and calibration of the tagging system of the GDH-Experiment at the accelerator facility ELSA in Bonn. The system consists of a C-type dipole magnet and a hodoscope of 65 scintillation counters which are operated pairwise in coincidence to form 64 tagging channels. Photons can be tagged in a range of 68-97% of the primary electron energy E-0. The energy resolution ranges from 0.2% to 0.6% of E-0. The time resolution is better than 165 ps. The system was operated at rates up to 5 x 10(6) photons/s in the full tagged energy range. The energy dependence of the photon definition probability was determined using several different methods and was found to agree well with calculations. (C) 2003 Elsevier Science B.V. All rights reserved.
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    Compton scattering by the proton
    (Elsevier Science Bv, 2001)
    Galler, G.
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    Lisin, V.
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    Kondratiev, R.
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    Massone, A. M.
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    Wolf, S.  
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    Ahrens, J.
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    Arends, H. J.
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    Beck, R.
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    Camen, M.
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    Capitani, G. P.
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    Grabmayr, P.
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    Hall, S. J.
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    Harter, Frauke V.
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    Hehl, T.
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    Jennewein, P.
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    Kossert, K.
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    L’vov, A. I.
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    Molinari, C.
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    Ottonello, P.
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    Peise, J.
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    Preobrajenski, I.
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    Proff, S.
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    Robbiano, A.
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    Sanzone, M.
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    Schumacher, M.
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    Schmitz, M.
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    Wissmann, F.
    Compton scattering by the proton has been measured over a wide range covering photon energies 250 MeV less than or similar to E-gamma less than or similar to 800 MeV and photon scattering angles 30 degrees less than or similar to theta (lab)(gamma) less than or similar to 150 degrees, using the tagged-photon facility at MAMI (Mainz) and the large-acceptance arrangement LARA. The data are in good agreement with the dispersion theory based on the SAID-SM99K parameterization of photo-meson amplitudes. From the subset of data between 280 and 360 MeV the resonance pion-photoproduction amplitudes were evaluated leading to the multipole E2/M1 ratio EMR(340 MeV) = (-1.6 +/- 0.4(stat+syst) +/- 0.2(model))% From all data below 455 MeV the proton's backward spin polarizability was determined to be gamma pi = (-37.9 +/- 0.6(stat+syst) +/- 3.5(model)) x 10(-4) fm(4). (C) 2001 Elsevier Science B.V. All rights reserved.
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    Compton scattering by the proton using a large-acceptance arrangement
    (Springer, 2001)
    Wolf, S.  
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    Lisin, V.
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    Kondratiev, R.
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    Massone, A. M.
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    Galler, G.
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    Ahrens, J.
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    Arends, H. J.
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    Beck, R.
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    Camen, M.
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    Capitani, G. P.
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    Grabmayr, P.
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    Harter, Frauke V.
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    Hehl, T.
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    Jennewein, P.
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    Kossert, K.
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    L’vov, A. I.
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    Molinari, C.
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    Ottonello, P.
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    Owens, R. O.
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    Peise, J.
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    Preobrajenskij, I.
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    Proff, S.
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    Robbiano, A.
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    Sanzone, M.
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    Schumacher, M.
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    Schmitz, M.
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    Wissmann, F.
    Compton scattering by the proton has been measured over a wide range covering photon energies 250 MeV less than or equal to E-gamma less than or similar to 800 MeV and photon scattering angles 30 degrees less than or similar to theta (lab)(gamma) less than or similar to 150 degrees, using the tagged-photon facility at MAMI (Mainz) and the large-acceptance arrangement LARA. The previously existing data base on proton Compton scattering is greatly enlarged by more than 700 new data points. The new data are interpreted in terms of dispersion theory based on the SAID-SM99K parametrization of photo-meson amplitudes. It is found that two-pion exchange in the t-channel is needed for a description of the data in the second resonance region. The data axe well represented if this channel is modeled by a single pole with the mass parameter m(sigma) approximate to 600 MeV. The asymptotic part of the spin-dependent amplitude is found to be well represented by pi (0) exchange in the t-channel. No indications of additional effects were found. Using the mass parameter m(sigma) of the two-pion exchange determined from the second resonance region and using the new global average for the difference of the electric and magnetic polarizabilities of the proton, alpha - beta = (10.5 +/- 0.9(stat+stat) +/- 0.7 model) x 10(-4) fm(3), as obtained from a recent experiment on proton Compton scattering below pion photoproduction threshold, a-backward spin polarizability of gamma (pi) = (-37.1 +/- 0.6(stat+syst) +/- 3.0model) x 10(-4) fm(4) has been determined from data of the first resonance region below 455 MeV. This value is in a good agreement with predictions of dispersion relations and chiral perturbation theory. From a subset of data between 280 and 360 MeV, the resonance pion photoproduction amplitudes were evaluated leading to a E2/M1 multipole ratio of the p --> Delta radiative transition of EMR(340 MeV) = (-1.7 +/- 0.4(stat+syst) +/- 0.2(model))%. It was found that this number is dependent on the parameterization of photo-meson amplitudes. With the MAID2K parameterization, an E2/M1 multipole ratio of EMR(340 MeV) = (-2.0 +/- 0.4(stat+syst) +/- 0.2(model))% is obtained.
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    Compton scattering from the deuteron and extracted neutron polarizabilities
    (Amer Physical Soc, 2003)
    Lundin, M.
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    Adler, J. O.
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    Boland, M.
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    Fissum, K.
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    Glebe, T.
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    Hansen, K.
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    Isaksson, L.
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    Kaltschmidt, O.
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    Karlsson, M.
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    Kossert, K.
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    Levchuk, M. I.
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    Lilja, P.
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    Lindner, Buko
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    L’vov, A. I.
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    Nilsson, B.
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    Oner, D. E.
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    Poech, C.
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    Proff, S.
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    Sandell, A.
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    Schroder, B.  
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    Schumacher, M.
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    Sims, D. A.
    Differential cross sections for Compton scattering from the deuteron were measured at MAX-Lab for incident photon energies of 55 and 66 MeV at nominal laboratory angles of 45degrees, 125degrees, and 135degrees. 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 the difference of the isospin-averaged nucleon polarizabilities, alpha(N) + beta(N) = 17.4 +/- 3.7 and alpha(N) - beta(N) = 6.4 +/- 2.4 (in units of 10(-4) fm(3)), have been determined. By combining the latter with the global-averaged value for 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 alpha(n) = 8.8 +/- 2.4(total) +/- 3.0(model) and beta(n) = 6.5 -/+ 2.4(total) -/+ 3.0(model), respectively.
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    Compton scattering from the free and bound proton above pi-threshold
    (Elsevier Science Bv, 2000)
    Wissmann, F.
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    Achenbach, P.
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    Ahrens, J.
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    Arends, H. J.
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    Beck, R.
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    Bilger, R.
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    Camen, M.
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    Capitani, G. P.
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    Caselotti, G.
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    Galler, G.
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    Grabmayr, P.
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    Harter, Frauke V.
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    Hehl, T.
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    Heid, E.
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    Hejny, V.
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    Jahn, Olaf  
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    Jennewein, P.
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    Kondratjev, R.
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    Kossert, K.
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    Kotulla, M.
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    Krusche, B.
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    Kuhr, V.
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    Lang, M.
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    Leukel, R.
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    Levchuk, M. I.
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    Lisin, V.
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    L’vov, A. I.
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    Massone, A. M.
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    Metag, V.
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    Natter, A.
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    Novotny, R.
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    de Leon, V. O.
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    Ottonello, P.
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    Peise, J.
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    Polonski, A.
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    Preobrashenskij, I.
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    Proff, S.
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    Rambo, F.
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    Robbiano, A.
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    Rosenkranz, D.
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    Sanzone, M.
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    Schilling, E.
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    Schmidt, A.
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    Schumacher, M.
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    Seitz, Bjoern
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    Siodlaczek, U.
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    Smend, F.
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    Stroher, H.
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    Vorwerk, Hilke
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    Walcher, T.
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    Weiss, J.
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    Wolf, M.
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    Zapadtka, F.
    The differential cross sections for Compton scattering from the proton have been measured at MAMI with three different detector setups. There is a good agreement among all the results. The theoretical calculation based on dispersion relations shows that there is no drastic change necessary in the parameters of this approach.
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    Structure of the nucleon investigated by Compton scattering
    (Elsevier Science Bv, 2001)
    Wolf, S.  
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    Lisin, V.
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    Kondratiev, R.
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    Massone, A. M.
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    Galler, G.
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    Ahrens, J.
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    Arends, H. J.
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    Beck, R.
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    Camen, M.
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    Capitani, G. P.
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    Grabmayr, P.
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    Hall, S. J.
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    Harter, Frauke V.
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    Hehl, T.
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    Jennewein, P.
    ;
    Kossert, K.
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    L’vov, A. I.
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    Molinari, C.
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    Ottonello, P.
    ;
    Peise, J.
    ;
    Preobrajenskij, I.
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    Proff, S.
    ;
    Robbiano, A.
    ;
    Sanzone, M.
    ;
    Schumacher, M.
    ;
    Schmitz, M.
    ;
    Wissmann, F.

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