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ProbingMo93mIsomer Depletion with an Isomer Beam
Physical Review Letters ( IF 8.6 ) Pub Date : 2022-06-17 , DOI: 10.1103/physrevlett.128.242502
S Guo 1, 2 , B Ding 1, 2 , X H Zhou 1, 2 , Y B Wu 3 , J G Wang 1, 2 , S W Xu 1, 2 , Y D Fang 1, 2 , C M Petrache 4 , E A Lawrie 5, 6 , Y H Qiang 1 , Y Y Yang 1, 2 , H J Ong 1, 2, 7, 8 , J B Ma 1, 2 , J L Chen 1, 2 , F Fang 1, 2 , Y H Yu 1, 2 , B F Lv 1 , F F Zeng 1 , Q B Zeng 1 , H Huang 1 , Z H Jia 1 , C X Jia 1 , W Liang 9 , Y Li 9 , N W Huang 10 , L J Liu 10 , Y Zheng 1, 2 , W Q Zhang 1, 2 , A Rohilla 1 , Z Bai 1, 2 , S L Jin 1, 2 , K Wang 1, 2 , F F Duan 1, 2 , G Yang 1, 2 , J H Li 1 , J H Xu 1 , G S Li 1, 2 , M L Liu 1, 2 , Z Liu 1, 2 , Z G Gan 1, 2 , M Wang 1, 2 , Y H Zhang 1, 2
Affiliation  

The isomer depletion of Mo93m was recently reported [Chiara et al., Nature (London) 554, 216 (2018)] as the first direct observation of nuclear excitation by electron capture (NEEC). However, the measured excitation probability of 1.0(3)% is far beyond the theoretical expectation. In order to understand the inconsistency between theory and experiment, we produce the Mo93m nuclei using the C12(Kr86,5n) reaction at a beam energy of 559 MeV and transport the reaction residues to a detection station far away from the target area employing a secondary beam line. The isomer depletion is expected to occur during the slowdown process of the ions in the stopping material. In such a low γ-ray background environment, the signature of isomer depletion is not observed, and an upper limit of 2×105 is estimated for the excitation probability. This is consistent with the theoretical expectation. Our findings shed doubt on the previously reported NEEC phenomenon and highlight the necessity and feasibility of further experimental investigations for reexamining the isomer depletion under low γ-ray background.

中文翻译:

用异构体光束探测 Mo93m 异构体耗尽

异构体消耗93最近有报道 [Chiara et al. , Nature (London) 554 , 216 (2018)] 作为电子捕获 (NEEC) 对核激发的首次直接观察。然而,测得的 1.0(3)% 的激发概率远远超出了理论预期。为了理解理论和实验之间的不一致,我们制作了93核使用C12(86,5n)以 559 MeV 的光束能量进行反应,并将反应残留物运送到远离目标区域的检测站,使用辅助光束线。异构体耗尽预计会在停止材料中离子的减速过程中发生。在如此低的γ-射线背景环境,未观察到异构体耗尽的特征,上限为2×10-5估计激励概率。这与理论预期一致。我们的研究结果对先前报道的 NEEC 现象提出了质疑,并强调了进一步实验研究以重新检查低电压下异构体耗尽的必要性和可行性。γ-射线背景。
更新日期:2022-06-17
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