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Analysis of nuclear resonance fluorescence excitation measured with LaBr$$_{3}$$(Ce) detectors near 2 MeV

2MeV領域における原子核共鳴蛍光散乱のLaBr$$_{3}$$(Ce)検出器による測定

Omer, M.*; Negm, H.*; 大垣 英明*; 大東 出*; 早川 岳人; Bakr, M.*; Zen, H.*; 堀 利匡*; 紀井 俊輝*; 増田 開*; 羽島 良一; 静間 俊行; 豊川 弘之*; 菊澤 信宏

Omer, M.*; Negm, H.*; Ogaki, Hideaki*; Daito, Izuru*; Hayakawa, Takehito; Bakr, M.*; Zen, H.*; Hori, Toshitada*; Kii, Toshiteru*; Masuda, Kai*; Hajima, Ryoichi; Shizuma, Toshiyuki; Toyokawa, Hiroyuki*; Kikuzawa, Nobuhiro

LaBr$$_{3}$$(Ce)シンチレータ検出器による原子核共鳴蛍光散乱(NRF)の測定性能を、ゲルマニウム検出器と比較して議論した。多くの核物質が励起準位をもつ2MeV領域に着目した。Duke大学の高強度$$gamma$$線施設(HIGS)において、2.12MeV$$gamma$$線をB$$_{4}$$C試料に照射し、$$^{11}$$Bの共鳴を測定した。測定データに対してSNIPアルゴリズムによるバックグラウンドの処理を行い、LaBr$$_{3}$$(Ce)検出器の測定限界を求めた。

The performance of LaBr$$_{3}$$ (Ce) to measure nuclear resonance fluorescence (NRF) excitations is discussedin terms of limits of detection and in comparison with high-purity germanium (HPGe)detectors near the 2 MeV region where many NRF excitation levels from special nuclear materials are located. The NRF experiment was performed at the High Intensity Gamma-ray Source (HIGS) facility of Duke University. The incident $$gamma$$-rays, of 2.12 MeV energy, hit a B$$_{4}$$C target to excite the $$^{11}$$B nuclei to the first excitation level. The statistical-sensitive non-linear peak clipping (SNIP) algorithm was implemented to eliminate theback ground and enhance the limits of detection for the spectra measured with LaBr$$_{3}$$ (Ce). Both detection and determination limits were deduced from the experimental data.

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パーセンタイル:53.77

分野:Instruments & Instrumentation

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