The COMPASS setup for physics with hadron beams
- Abbon, P.
- Adolph, C.
- Akhunzyanov, R.
- Alexandrov, Yu.
- Alexeev, M.G.
- Alexeev, G.D.
- Amoroso, A.
- Andrieux, V.
- Anosov, V.
- Austregesilo, A.
- Badełek, B.
- Balestra, F.
- Barth, J.
- Baum, G.
- Beck, R.
- Bedfer, Y.
- Berlin, A.
- Bernhard, J.
- Bicker, K.
- Bielert, E.R.
- Bieling, J.
- Birsa, R.
- Bisplinghoff, J.
- Bodlak, M.
- Boer, M.
- Bordalo, P.
- Bradamante, F.
- Braun, C.
- Bressan, A.
- Büchele, M.
- Burtin, E.
- Capozza, L.
- Ciliberti, P.
- Chiosso, M.
- Chung, S.U.
- Cicuttin, A.
- Colantoni, M.
- Cotte, D.
- Crespo, M.L.
- Curiel, Q.
- Dafni, T.
- Dalla Torre, S.
- Dasgupta, S.S.
- Dasgupta, S.
- Denisov, O.Yu.
- Desforge, D.
- Dinkelbach, A.M.
- Donskov, S.V.
- Doshita, N.
- Duic, V.
- Dünnweber, W.
- Durand, D., Dominique
- Dziewiecki, M.
- Efremov, A.
- Elia, C.
- Eversheim, P.D.
- Eyrich, W.
- Faessler, M.
- Ferrero, A.
- Finger, M.
- Fischer, H.
- Franco, C.
- Du Fresne von Hohenesche, N.
- Friedrich, J.M.
- Frolov, V.
- Gatignon, L.
- Gautheron, F.
- Gavrichtchouk, O.P.
- Gerassimov, S.
- Geyer, R.
- Giganon, A.
- Gnesi, I.
- Gobbo, B.
- Goertz, S.
- Gorzellik, M.
- Grabmüller, S.
- Grasso, A.
- Gregori, M.
- Grube, B.
- Grussenmeyer, T.
- Guskov, A.
- Haas, F.
- von Harrach, D.
- Hahne, D.
- Hashimoto, R.
- Heinsius, F.H.
- Herrmann, F.
- Hinterberger, F.
- Höppner, Ch.
- Horikawa, N.
- D׳hose, N.
- Huber, S.
- Ishimoto, S.
- Ivanov, A.
- Ivanshin, Yu.
- Iwata, T.
- Jahn, R.
- Jary, V.
- Jasinski, P.
- Jörg, P.
- Joosten, R.
- Kabuss, E.
- Ketzer, B.
- Khaustov, G.V.
- Khokhlov, Yu.A.
- Kisselev, Yu.
- Klein, F.
- Klimaszewski, K.
- Koivuniemi, J.H.
- Kolosov, V.N.
- Kondo, K.
- Königsmann, K.
- Konorov, I.
- Konstantinov, V.F.
- Kotzinian, A.M.
- Kouznetsov, O.
- Krämer, M.
- Kroumchtein, Z.V.
- Kuchinski, N.
- Kuhn, R.
- Kunne, F.
- Kurek, K.
- Kurjata, R.P.
- Lednev, A.A.
- Lehmann, A.
- Levillain, M.
- Levorato, S.
- Lichtenstadt, J.
- Maggiora, A.
- Magnon, A.
- Makke, N.
- Mallot, G.K.
- Marchand, C.
- Marroncle, J.
- Martin, A.
- Marzec, J.
- Matousek, J.
- Matsuda, H.
- Matsuda, T.
- Menon, G.
- Meshcheryakov, G.
- Meyer, W.
- Michigami, T.
- Mikhailov, Yu.V.
- Miyachi, Y.
- Moinester, M.A.
- Nagaytsev, A.
- Nagel, T.
- Nerling, F.
- Neubert, S.
- Neyret, D.
- Nikolaenko, V.I.
- Novy, J.
- Nowak, W.-D.
- Nunes, A.S.
- Olshevsky, A.G.
- Orlov, I.
- Ostrick, M.
- Panknin, R.
- Panzieri, D.
- Parsamyan, B.
- Paul, S.
- Pesaro, G.
- Pesaro, V.
- Peshekhonov, D.V.
- Pires, C.
- Platchkov, S.
- Pochodzalla, J.
- Polyakov, V.A.
- Pretz, J.
- Quaresma, M.
- Quintans, C.
- Ramos, S.
- Regali, C.
- Reicherz, G.
- Reymond, J-M.
- Rocco, E.
- Rossiyskaya, N.S.
- Rousse, J.-Y.
- Ryabchikov, D.I.
- Rychter, A.
- Samartsev, A.
- Samoylenko, V.D.
- Sandacz, A.
- Sarkar, S.
- Savin, I.A.
- Sbrizzai, G.
- Schiavon, P.
- Schill, C.
- Schlüter, T.
- Schmidt, K.
- Schmieden, H.
- Schönning, K.
- Schopferer, S.
- Schott, M.
- Shevchenko, O.Yu.
- Silva, L.
- Sinha, L.
- Sirtl, S.
- Slunecka, M.
- Sosio, S.
- Sozzi, F.
- Srnka, A.
- Steiger, L.
- Stolarski, M.
- Sulc, M.
- Sulej, R.
- Suzuki, H.
- Szabelski, A.
- Szameitat, T.
- Sznajder, P.
- Takekawa, S.
- Terça, G.
- Wolbeek, J. Ter
- Tessaro, S.
- Tessarotto, F.
- Thibaud, F.
- Tskhay, V.
- Uhl, S.
- Uman, I.
- Virius, M.
- Wang, L.
- Weisrock, T.
- Weitzel, Q.
- Wilfert, M.
- Windmolders, R.
- Wollny, H.
- Zaremba, K.
- Zavertyaev, M.
- Zemlyanichkina, E.
- Ziembicki, M.
- Zink, A.
DOIAbstract
International audienceThe main characteristics of the COMPASS experimental setup for physics with hadron beams are described. This setup was designed to perform exclusive measurements of processes with several charged and/or neutral particles in the final state. Making use of a large part of the apparatus that was previously built for spin structure studies with a muon beam, it also features a new target system as well as new or upgraded detectors. The hadron setup is able to operate at the high incident hadron flux available at CERN. It is characterised by large angular and momentum coverages, large and nearly flat acceptances, and good two and three-particle mass resolutions. In 2008 and 2009 it was successfully used with positive and neg...
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