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Simulation of the interaction of galactic cosmic ray protons with meteoroids: On the production of 3H and light noble gas isotopes in isotropically irradiated thick gabbro and iron targets

机译:银河系宇宙射线质子与流星体相互作用的模拟:在各向同性辐照的厚辉石和铁靶中产生3H和轻质惰性气体同位素

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Thick spherical targets, one made of gabbro (R = 25 cm) and one made of iron (R= 10 cm), were irradiated isotropically with 1.6 GeV protons at Laboratoire National Saturne (LNS)/Saclay to simulate the interactions of galactic cosmic ray protons with meteoroids in space. At various depths, both artificial meteoroids contained a large number of high-purity, single-element target foils and chemical compounds of up to 28 target elements. In these individual target foils, the elemental production rates of radionuclides and noble gas isotopes were measured. Here, we report the results for the light noble gas isotopes ~(3,4)He, ~(20,21,22)Ne, and ~(36,38,39)Arforthe mostcosmochemically relevant target elements as well as for some meteoritic material from Jilin, Farmington, and Cape York. From ~3He analyses done several years apart, ~3H diffusive losses during sample storage have been obtained, and direct as well as cumulative ~3He production rates for O, Mg, Al, Si, Fe, Ni, and the meteoritic material are given. Losses by diffusion of tritium from metallic Mg and Fe are found to occur on time scales of months, while metallic Al, Si, and stone meteorites are much more retentive. The production rate ratios P(~3H)/P(~3He)_d obtained in the simulation experiments are 0.73, 1.28, and 1.16 for O, Al, and Si, respectively. These rates are based on our best knowledge about the ~3H and ~3He production rates and should, therefore, replace data published earlier (Leya et al. 2000a). The earlier calculations for ~4He, ~(20,21,22)Ne, and ~(36,38,39)Ar remain valid. The new modeled correlation ~3He_(cum)/~(21)Ne versus ~(22)Ne/~(21)Ne for chondrites exposed to cosmic rays with an energy spectrum characterized by a modulation parameter of = 650 MeV is in fair agreement with the empirical relationship ("Berne plot"). However, for small meteorites and little shielding in larger ones, there are systematic differences that most likely are due to an underestimation of the spallogenic ~(22)Ne/~(21)Ne ratio by ~2%.
机译:用1.6 GeV质子向各向同性辐照了厚球形目标,其中一个由辉长球(R = 25 cm)制成,一个由铁制成(R = 10 cm),在国家实验室Saturne(LNS)/ Saclay上各向同性地照射了1.6 GeV质子,以模拟银河系宇宙射线的相互作用在太空中有流星体的质子。在不同深度,两种人造流星体都包含大量高纯度的单元素靶箔和多达28种靶元素的化合物。在这些单独的目标箔中,测量了放射性核素和稀有气体同位素的元素生产率。在这里,我们报告了轻稀有气体同位素〜(3,4)He,〜(20,21,22)Ne和〜(36,38,39)Ar的结果,这是与宇宙化学最相关的目标元素以及某些陨石的吉林,法明顿和约克角的资料。从相隔数年的〜3He分析中,获得了样品存储过程中〜3H的扩散损失,并给出了O,Mg,Al,Si,Fe,Ni和陨石材料的直接和累计〜3He生产率。 M从金属镁和铁中扩散出来的ses损失在数月的时间尺度上发生,而金属铝,硅和陨石则更具保留性。在模拟实验中获得的生产率比率P(〜3H)/ P(〜3He)_d对于O,Al和Si分别为0.73、1.28和1.16。这些速率是基于我们对〜3H和〜3He生产率的最佳了解,因此,应取代先前发布的数据(Leya等人2000a)。 〜4He,〜(20,21,22)Ne和〜(36,38,39)Ar的早期计算仍然有效。新的建模关联〜3He_(cum)/〜(21)Ne与〜(22)Ne /〜(21)Ne有关暴露于具有以 = 650 MeV调制参数为特征的能谱的宇宙射线的球粒陨石与经验关系完全一致(“伯恩图”)。但是,对于小陨石和大陨石,几乎没有系统差异,这很可能是由于散裂性〜(22)Ne /〜(21)Ne比被低估了约2%。

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