Design and construction of the cylindrical drift chamber for the COMET Phase-I experiment

A. Sato a, H. Yoshida a b, M. Moritsu c, X. Jiang d e, Y. Kuno a b, H.-B. Li d e, W.-G. Li d e 1, Y. Matsuda a, H. Miao d e, Y. Nakamura a, Y. Nakatsugawa g, Y. Nakazawa h, S. Ohta a, K. Okinaka a, H. Sakamoto a, M.L. Wong a 2, T.S. Wong a, C. Wu d f, T.-Y. Xing d e, T. Yamane a, Y. Yuan d e, J. Zhang d e, Y. Zhang d, Z.-K. Zhang d e

Department of Physics, Osaka University, 1-1 Machikaneyama, Toyonaka, 560-0043, Osaka, Japan
Research Center for Nuclear Physics, Osaka University, 10-1 Mihogaoka, Suita, 567-0047, Osaka, Japan
Department of Physics, Kyushu University, 744 Motooka, Nishi-ku, 819-0395, Fukuoka, Japan
Institute of High Energy Physics, Chinese Academy of Sciences, 100049, Beijing, China
e University of Chinese Academy of Sciences, 100049, Beijing, China
f Spallation Neutron Source Science Center, 523808, Dongguan, China
g Wakayama Medical University, 811-1 Kimiidera, Wakayama, 641-8509, Wakayama, Japan
h KEK, 1-1 Oho, Tsukuba, 305-0801, Ibaraki, Japan
Nucl.Instrum.Meth.A 1069 (2024) 169926
9/30/24

COMET is an experiment at J-PARC that searches for the charged lepton flavor violating process of neutrino-less muon-to-electron conversion ( conversion) in a muonic atom. The COMET Phase-I experiment, which represents the first stage of its staged approach, utilizes the cylindrical drift chamber (CDC) as the main detector to measure the momentum of electrons emitted from conversion in a 1 T magnetic field. The CDC is designed for optimal performance to achieve the best momentum resolution and effectively separate the conversion electron signal from background signals. This design entails adapting He:i-C4H10 (90:10) as its chamber gas and employing an all-stereo wire configuration. This document provides a comprehensive overview of the CDC detector, encompassing design considerations, mechanical structure, construction methodologies, and results of performance evaluations conducted using cosmic-rays.

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