Extraction and trapping of <sup>229m</sup>Th ions for measuring nuclear-decay half-lives of various ionic species of <sup>229m</sup>Th and observing electronic bridge process
ORAL
Abstract
The first excited state of the 229Th nucleus, 229mTh, has a low excitation energy of 8.3 eV, which allows the variation of its decay mode (internal conversion (IC) [1], gamma-ray emission [2], and electronic bridge (EB)) depending on the chemical environment. The EB process, which is an exotic nuclear decay through the transition of an atomic electron, has never been observed thus far. The half-life of the EB process is expected to largely different from other decay modes; hence, we aim to measure the nuclear-decay half-lives of some candidates such as 229mTh+ and 229ThO2+ to find the EB process of 229mTh.
We developed an extraction and trapping apparatus for 229mTh ions. 229mTh2+,3+ ions emitted from a 233U source are extracted by a radiofrequency-carpet gas cell into an ion trap, where 229mTh+ and molecular 229mTh ions are produced by chemical reactions with reactive gases. The produced ions are then extracted, mass-separated, and placed on a multichannel plate (MCP) detector. The half-lives of 229mTh can be determined from the number of trapped 229mTh (the number of IC electrons measured by the MCP detector) as a function of the trapping time.
We successfully extracted 229Th3+,2+ and observed the IC electrons emitted from 229mTh neutralized on a MCP detector. Moreover, we were able to produce 229Th+ and 229ThO2+ by the reaction with impurities in Ar gas. We will soon try to measure the half-lives of these 229mTh species.
[1] L. von der Wense et al., Nature 533, 47 (2016).
[2] S. Kraemer et al, Nature 617, 706 (2023).
We developed an extraction and trapping apparatus for 229mTh ions. 229mTh2+,3+ ions emitted from a 233U source are extracted by a radiofrequency-carpet gas cell into an ion trap, where 229mTh+ and molecular 229mTh ions are produced by chemical reactions with reactive gases. The produced ions are then extracted, mass-separated, and placed on a multichannel plate (MCP) detector. The half-lives of 229mTh can be determined from the number of trapped 229mTh (the number of IC electrons measured by the MCP detector) as a function of the trapping time.
We successfully extracted 229Th3+,2+ and observed the IC electrons emitted from 229mTh neutralized on a MCP detector. Moreover, we were able to produce 229Th+ and 229ThO2+ by the reaction with impurities in Ar gas. We will soon try to measure the half-lives of these 229mTh species.
[1] L. von der Wense et al., Nature 533, 47 (2016).
[2] S. Kraemer et al, Nature 617, 706 (2023).
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Presenters
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Yudai Shigekawa
RIKEN, RIKEN Nishina Center
Authors
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Yudai Shigekawa
RIKEN, RIKEN Nishina Center
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Atsushi Yamaguchi
RIKEN
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Katsuyuki Tokoi
Osaka University
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Nozomi Sato
RIKEN Nishina Center
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Michiharu Wada
KEK Wako Nuclear Science Center, High Energy Accelerator Research Organization (KEK), KEK, WNSC, IPNS, High Energy Accelerator Research Organization (KEK), Wako Nuclear Science Center (WNSC), KEK, Japan, WNSC, KEK, Wako Nuclear Science Center (WNSC), KEK
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Hiromitsu Haba
RIKEN, RIKEN Nishina center, Nishina Center for Accelerator-Based Science, RIKEN