2017年第64回応用物理学会春季学術講演会

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一般セッション(口頭講演)

2 放射線 » 2.1 放射線物理一般・検出器基礎

[14p-E204-1~21] 2.1 放射線物理一般・検出器基礎

2017年3月14日(火) 12:30 〜 18:15 E204 (E204)

越水 正典(東北大)、南戸 秀仁(金沢工大)、神野 郁夫(京大)

13:30 〜 13:45

[14p-E204-5] Measurements of Electron Response and Average Energy Required per Scintillation Photon in Plastic Scintillators for Gamma Rays (II)

〇(D)Tran Ngan NguyenThuy1、Sasaki Shinichi1,2、Sanami Toshiya1,2、Kishimoto Yuji1,2、Shibamura Eido3 (1.SOKENDAI、2.KEK、3.Waseda Univ.)

キーワード:plastic scintillators, scintillation yield, Compton Coincidence Technique

Previously, we have introduced preliminary data of the relative scintillation yield per unit energy deposited by electrons (called as “electron response”), which are measured by Compton Coincidence Technique (CCT), and of average energy required per scintillation photon Ws in plastic scintillators (EJ-200, EJ-212, EJ-252). In this study, Ws values in these plastic scintillators are re-evaluated in consideration of photon transport evaluation in a scintillator-photomultiplier tube system. Ws is defined as E / Nph, where E is the deposited energy in the scintillator and Nph is the number of scintillation photons produced. New data of deposited energies E in these plastic scintillators are measured by CCT and Nph is calculated relatively to the Nph in a CsI(Tl) scintillator. The Nph in the CsI(Tl) is determined from the combination of the absolute number of photoelectrons (measured for a 2-inch diameter and 2-inch length crystal coupling to a photomultiplier tube (PMT) operated as a photodiode, the system is irradiated with gamma rays), the calculation of collection efficiency of scintillation photons at the PMT photocathode using Monte Carlo simulations and experimental determination of photon-to-photoelectron conversion efficiency at the PMT photocathode. Employing Ws values, the absolute light yield of plastic scintillators can be evaluated and then compared with light yields of other scintillators.