Bulletin of the American Physical Society
6th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Sunday–Friday, November 26–December 1 2023; Hawaii, the Big Island
Session 2WGB: New Detector Technologies for Radioactive Isotope Beam Facilities II
4:00 PM–5:30 PM,
Sunday, November 26, 2023
Hilton Waikoloa Village
Room: Queens 6
Chair: Daniel Bazin, Michigan State University
Abstract: 2WGB.00002 : Xenon-gas ionization chamber for improving high-Z beam particle identification*
4:30 PM–5:00 PM
Presenter:
Masahiro Yoshimoto
(RIKEN Nishina Center)
Authors:
Masahiro Yoshimoto
(RIKEN Nishina Center)
Naoki Fukuda
(RIKEN Nishina Center)
Riku Matsumura
(Saitama University)
Daiki Nishimura
(Tokyo City University)
Hideaki Otsu
(RIKEN Nishina Center)
Yohei Shimizu
(RIKEN Nishina Center)
Toshiyuki Sumikama
(RIKEN Nishina Center)
Hiroshi Suzuki
(RIKEN Nishina Center)
Hiroyuki Takahashi
(Tokyo City University)
Hiroyuki Takeda
(RIKEN Nishina Center)
Junki Tanaka
(RIKEN Nishina Center)
Koichi Yoshida
(RIKEN Nishina Center)
The insufficient Z resolution is due to the increased energy loss straggling due to charge fluctuations. The Z is estimated from the particle velocity and the energy loss of the ions. The energy loss is measured using an ionization chamber (IC) at BigRIPS. The conventional IC gas, P-10 (argon 90% and methane 10%), causes a large energy loss straggling due to insufficient charge state changes.
To solve this problem, we switched from the conventional P-10 gas to xenon-based gas (xenon 70% and methane 30%) to increase the number of charge state changes. According to the charge fluctuation cross-section, the xenon-based gas increases the number of charge state changes by approximately one order of magnitude compared to P-10 gas. By reducing the energy loss straggling caused by the charge fluctuation, the Z resolution is expected to improve.
The Z resolutions of the xenon-based gas IC and the P-10 gas IC were evaluated using a cocktail beam with Z=40-90 at 200-250 MeV/u. The results of the xenon-based gas IC showed a Z resolution comparable to that of the P-10 gas IC at Z<70 and a remarkable improvement in Z resolution at Z>70. The Z resolution (FWHM) at Z=84-88 was 1.3 for the P-10 gas and 0.8 for the xenon-based gas, which is a 1.7-fold improvement over the P-10 gas. The simulation of the charge fluctuation explained this improvement. In conclusion, the xenon-based gas IC was highly effective for Z identification. The separation and supply of heavy RI beams using the xenon-based gas IC have already been started at RIBF.
*This work has been supported by the JSPS A3 Foresight Program, ``Nuclear Physics in the 21st Century''.
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