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  1. 原著論文

Monte Carlo simulation to optimize measurement geometry of continuous air monitor with Si semiconductor detector

https://repo.qst.go.jp/records/2002780
https://repo.qst.go.jp/records/2002780
09024bec-b218-4ece-9d4a-c0404e09c9e6
アイテムタイプ 学術雑誌論文 / Journal Article(1)
公開日 2026-02-17
タイトル
タイトル Monte Carlo simulation to optimize measurement geometry of continuous air monitor with Si semiconductor detector
言語 en
言語
言語 eng
資源タイプ
資源タイプ識別子 http://purl.org/coar/resource_type/c_6501
資源タイプ journal article
著者 Yuki Tamakuma

× Yuki Tamakuma

Yuki Tamakuma

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Hiroki Hashimoto

× Hiroki Hashimoto

Hiroki Hashimoto

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Manaya Taoka

× Manaya Taoka

Manaya Taoka

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Ryohei Yamada

× Ryohei Yamada

Ryohei Yamada

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Kazuki Iwaoka

× Kazuki Iwaoka

Kazuki Iwaoka

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Yasutaka Omori

× Yasutaka Omori

Yasutaka Omori

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Masahiro Hosoda

× Masahiro Hosoda

Masahiro Hosoda

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Shinji Tokonami

× Shinji Tokonami

Shinji Tokonami

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抄録
内容記述タイプ Abstract
内容記述 One of the challenges in real-time monitoring of airborne alpha-emitting radionuclides using Continuous Air Monitors (CAMs) is to discriminate alpha particles emitted by artificial radionuclides from those emitted by natural radionuclides, as the alpha energy spectrum is easily degraded due to its high stopping power. Although the measurement geometry significantly affects the alpha energy spectrum, there are no reports that have investigated the optimized geometry. This study conducted a Monte Carlo simulation to optimize the measurement geometry of the CAMs. The CAM was modelled using a radiation transport simulation code, and the counting efficiencies for 218Po and 239Pu and the overlapping ratio were simulated. The Minimum Detectable Concentration (MDC) of 239Pu was then estimated as an indicator to optimize the geometry. Although a constant counting efficiency is generally used for the same geometry regardless of the alpha energy, the counting efficiency differed up to ∼0.04 by the alpha energy depending on the measurement geometry. The overlapping ratio for a 50-mm diameter detector ranged from 0.22 to 0.35, while those for a 25-mm diameter detector was below 0.25. This discrepancy is because of the incident angle distribution biased towards large angles. The lowest MDC was estimated to be ∼3 Bq m−3 at 20 L min−1 under 25 Bq m−3 of 218Po. The MDC was low for small filter diameters and Filter-to-Detector Distances (FDDs) under most of the simulated conditions. The results indicate that a shorter filter diameter and FDD would be preferable for alpha spectrometry under normal air pressure.
書誌情報 Radiation Physics and Chemistry

巻 241, p. 113507, 発行日 2025-12
DOI
識別子タイプ DOI
関連識別子 10.1016/j.radphyschem.2025.113507
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