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Baldini, A. M.; Benmansour, H.; Boca, G.; Cavoto, G.; Cei, F.; Chiappini, M.; Chiarello, G.; Corvaglia, A.; Cuna, F.; Francesconi, M.; Galli, L.; Grancagnolo, F.; Grandoni, E. G.; Grassi, M.; Hildebrandt, M.; Ignatov, F.; Meucci, M.; Molzon, W.; Nicolò, D.; Oya, A.; Palo, D.; Panareo, M.; Papa, A.; Raffaelli, F.; Renga, F.; Signorelli, G.; Tassielli, G. F.; Uchiyama, Y.; Venturini, A.; Vitali, B.; Voena, C.
The European physical journal. C, Particles and fields, 05/2024, Volume: 84, Issue: 5Journal Article
The cylindrical drift chamber is the most innovative part of the MEG II detector, the upgraded version of the MEG experiment. The MEG II chamber differs from the MEG one because it is a single volume cylindrical structure, instead of a segmented one, chosen to improve its resolutions and efficiency in detecting low energy positrons from muon decays at rest. In this paper, we show the characteristics and performances of this fundamental part of the MEG II apparatus and we discuss the impact of its higher resolution and efficiency on the sensitivity of the MEG II experiment. Because of its innovative structure and high quality resolution and efficiency the MEG II cylindrical drift chamber will be a cornerstone in the development of an ideal tracking detector for future positron-electron collider machines.
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