论文标题

$^{39} ar $和$^{42} ar $的宇宙生产评估,用于稀有事件物理学

Evaluation of cosmogenic production of $^{39}Ar$ and $^{42}Ar$ for rare-event physics using underground argon

论文作者

Zhang, Chao, Mei, Dongming

论文摘要

在$^{39} ar $和$^{42} ar $的宇宙源性活动较低的地下氩气(UAR)已被计划为检测闪烁光和电荷收集的探测器,并使用时间投影室进行暗物质搜索,并作为暗物质探测器作为抑制背景的兽医探测器,以抑制中性beta beta beta beta depa beta debae debain beta decay(0 $ $ z)$名$ sm)。长寿命的放射性同位素,$^{39} ar $和$^{42} ar $,当UAR从深井中抽出时,也可以在表面上产生。了解AR中寿命长的同位素的产生对于将UAR用于暗物质很重要,而在其生产,运输和储存方面,0 $νββ$实验很重要。使用GEANT4,对于给定的宇宙射线MUON,中子和质子能谱,使用GEANT4模拟了海平面宇宙射线的AR暴露。我们报告了$^{39} ar $,$^{42} ar $的模拟宇宙生产速率,以及从快速中性子,高能量muons和高能量质子的海平面的其他长期同位素。 938.53/kg $ _ {ar} \ cdot $ DAY和5.81 $ \ times $ 10 $^{ - 3} $^{ - 3} $/kg $ _ {ar} \ cdot $ day for $^{39} $ ar和$^{42} $的总生产率。利用这些生产率,我们设定了954天的时间限制,该时间限制受$^{39} $ ar的产生,使UAR在损害暗物质实验的敏感性之前表面保持表面。同样,对于0 $νβ$实验的$^{42} $ AR的产生,限制了1702天的时间限制。

Underground argon (UAr) with lower cosmogenic activities of $^{39}Ar$ and $^{42}Ar$ has been planned as a detector in detecting scintillation light and charge collection using time projection chambers for dark matter searches and as a veto detector in suppressing backgrounds for neutrinoless double beta decay (0$νββ$) experiments. Long-lived radioactive isotopes, $^{39}Ar$ and $^{42}Ar$, can also be produced on the surface when UAr is pumped out from a deep well. Understanding the production of long-lived isotopes in Ar is important for utilizing UAr for dark matter and 0$νββ$ experiments in terms of its production, transportation, and storage. Ar exposure to cosmic rays at sea-level is simulated using Geant4 for a given cosmic ray muon, neutron, and proton energy spectrum. We report the simulated cosmogenic production rates of $^{39}Ar$, $^{42}Ar$, and other long-lived isotopes at sea-level from fast neutrons, high energy muons, and high energy protons. Total production rates of 938.53/kg$_{Ar}\cdot$day and 5.81$\times$10$^{-3}$/kg$_{Ar}\cdot$day for $^{39}$Ar and $^{42}$Ar are found from our simulation. Utilizing these production rates, we set a time limit of 954 days constrained by the production of $^{39}$Ar for UAr to be on the surface before it compromises the sensitivity for a dark matter experiment. Similarly, a time limit of 1702 days constrained by the production of $^{42}$Ar is found for a 0$νββ$ experiment.

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