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A time-of-propagation (TOP) counter is a <\/p>\n","protected":false},"featured_media":0,"template":"","tags":[],"seminar_category":[58],"acf":{"s_now_accepting":true,"s_date_order":"2014-06-11 17:30:00","s_date_end":null,"s_date_text":"","s_text":"Tomokatsu Hayakawa","s_place":"KMI Science Symposia (ES635)","s_place_other":"","s_categoryother":"","s_poster":"","s_poster2":"
\ncompact ring imaging Cherenkov detector proposed for charged particle
\nidentification (PID) in the barrel region of the Belle II detector. The design goal of the TOP counter is to
\nachieve good K\/$pi$ separation in the momentum range up to 4 GeV\/c. In the TOP counter, Cherenkov photons
\nproduced inside a quartz radiator are measured with an array of Micro Channel
\nPlate Photomultiplier Tubes (MCP-PMTs).
\nThe Cherenkov angle is reconstructed using the propagation times and
\ndetected positions. In this talk, we
\nwill summarize current detector development activities and plans towards
\ninstallation in early 2015.<\/span><\/p>\n