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Production of selected cosmogenic radionuclides by muons: 2. Capture of negative muons

机译:介子产生选定的宇宙放射性核素:2.捕获负介子

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摘要

We have determined the production yields for radionuclides in Al_2O_3, SiO_2, S, Ar, K_2SO_4, CaCO_3, Fe, Ni and Cu targets, which were irradiated with slow negative muons at the Paul Scherrer Institute in Villigen (Switzerland). The fluences of the stopped negative muons were determined by measuring the muonic X-rays. The concentrations of the long-lived and short-lived radionuclides were measured with accelerator mass spectrometry (AMS) and γ-spectroscopy, respectively. Special emphasis was put on the radionuclides ~(10)Be, ~(14)C and ~(26)Al produced in quartz targets, ~(26)Al in Al_2O_3 and S targets, ~(36)Cl in K_2SO_4 and CaCO_3 targets, and ~(53)Mn in Fe_2O_3 targets. These targets were selected because they are also the naturally occurring target minerals for cosmic ray interactions in typical rocks. We also present results of calculations for depth-dependent production rates of radionuclides produced after cosmic ray μ~- capture, as well as cosmic ray-induced production rates of geologically relevant radionuclides produced by the nucleonic component, by μ~- capture, by fast muons and by neutron capture.
机译:我们确定了Al_2O_3,SiO_2,S,Ar,K_2SO_4,CaCO_3,Fe,Ni和Cu靶标中的放射性核素的产率,这些靶材在瑞士Villigen的Paul Scherrer研究所用缓慢的负介子进行了辐照。停止的负子的通量是通过测量子X射线来确定的。长寿命和短寿命放射性核素的浓度分别通过加速器质谱(AMS)和γ谱仪测量。特别强调了石英靶中产生的放射性核素〜(10)Be,〜(14)C和〜(26)Al,Al_2O_3和S目标中的〜(26)Al,K_2SO_4和CaCO_3中的〜(36)Cl和〜(53)Mn在Fe_2O_3靶中。选择这些目标的原因是它们也是典型岩石中宇宙射线相互作用的天然目标矿物。我们还介绍了宇宙射线μ〜-捕获后产生的与深度有关的放射性核素的生产速率的计算结果,以及由核子组分,μ〜-捕获,快速生成的与核子组分产生的地质相关放射性核素的宇宙射线诱导的生产率。介子并被中子俘获。

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