New limit on two neutrino electron capture with positron emission in 106Cd

O. Polischuk, P. Belli, R. Bernabei, V. Brudanin, F. Cappella, V. Caracciolo, R. Cerulli, F. Danevich, A. Incicchitti, D. Kasperovych, V. Kobychev, V. Tretyak, M. Zarytskyy
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引用次数: 5

Abstract

An experiment to search for double beta processes in 106Cd is in progress with the help of 106CdWO4 crystal scintillator (enriched in 106Cd to 66%) in coincidence with two large volume CdWO4 crystal scintillators in close geometry at the Gran Sasso Underground Laboratory. The time resolution of the set-up was analyzed, and the methods of pulse-shape discrimination of α and γ(β) events was applied to estimate the radioactive contamination of the crystal and to reduce the background counting rate. The possible double beta decay processes and the background components have been simulated by a Monte Carlo method with GEANT4. The experimental sensitivity is approaching the theoretical predictions for the two-neutrino electron capture with positron emission in 106Cd: lim T1/2≥4×1021 yr at 90% C.L. (the best previous limit was established in the previous stage of the experiment as T1/2≥1.1× 1021 yr, while the theoretical predictions are in the region of T1/2∼1021−1022 yr).An experiment to search for double beta processes in 106Cd is in progress with the help of 106CdWO4 crystal scintillator (enriched in 106Cd to 66%) in coincidence with two large volume CdWO4 crystal scintillators in close geometry at the Gran Sasso Underground Laboratory. The time resolution of the set-up was analyzed, and the methods of pulse-shape discrimination of α and γ(β) events was applied to estimate the radioactive contamination of the crystal and to reduce the background counting rate. The possible double beta decay processes and the background components have been simulated by a Monte Carlo method with GEANT4. The experimental sensitivity is approaching the theoretical predictions for the two-neutrino electron capture with positron emission in 106Cd: lim T1/2≥4×1021 yr at 90% C.L. (the best previous limit was established in the previous stage of the experiment as T1/2≥1.1× 1021 yr, while the theoretical predictions are in the region of T1/2∼1021−1022 yr).
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106Cd中正电子发射的两个中微子电子捕获的新极限
在格兰萨索地下实验室,利用106CdWO4晶体闪烁体(富106Cd至66%)与两个大体积CdWO4晶体闪烁体在近几何位置重合,进行了一项寻找106Cd双β过程的实验。分析了装置的时间分辨率,并采用α和γ(β)事件的脉冲形状判别方法来估计晶体的放射性污染并降低背景计数率。利用GEANT4软件对可能的双β衰变过程和背景分量进行了蒙特卡罗模拟。实验灵敏度接近106Cd中正电子发射的双中微子电子捕获的理论预测:在90% C.L.下T1/2≥4×1021 yr(实验前阶段建立的最佳极限为T1/2≥1.1× 1021 yr,而理论预测范围为T1/2 ~ 1021−1022 yr)。在格兰萨索地下实验室,利用106CdWO4晶体闪烁体(富106Cd至66%)与两个大体积CdWO4晶体闪烁体在近几何位置重合,进行了一项寻找106Cd双β过程的实验。分析了装置的时间分辨率,并采用α和γ(β)事件的脉冲形状判别方法来估计晶体的放射性污染并降低背景计数率。利用GEANT4软件对可能的双β衰变过程和背景分量进行了蒙特卡罗模拟。实验灵敏度接近106Cd中正电子发射的双中微子电子捕获的理论预测:在90% C.L.下T1/2≥4×1021 yr(实验前阶段建立的最佳极限为T1/2≥1.1× 1021 yr,而理论预测范围为T1/2 ~ 1021−1022 yr)。
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