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首页> 外文期刊>Earth and Planetary Science Letters: A Letter Journal Devoted to the Development in Time of the Earth and Planetary System >Long-term cosmogenic ~3He production rates (152 ka-1.35 Ma) from ~(40)Ar/~(39)Ar dated basalt flows at 29°N latitude
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Long-term cosmogenic ~3He production rates (152 ka-1.35 Ma) from ~(40)Ar/~(39)Ar dated basalt flows at 29°N latitude

机译:〜(40)Ar /〜(39)Ar年月玄武岩流在纬度29°N时的长期宇宙成因〜3He生产率(152 ka-1.35 Ma)

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摘要

A set of time integrated cosmogenic ~3He production rates in olivines for the last 1.35 Ma are presented. We investigated three basaltic lava flow tops from Lanzarote, Canary Islands, Spain, The ~(40)Ar/~(39)Ar ages determined for those basalt flows by incremental laser heating of leached groundmass samples are 152 ± 26 ka, 281 ± 19 ka and 1.35 ± 0.01 Ma (±2σ). Three or four different olivine phenocryst samples have been analyzed from each flow for their cosmogenic ~3He abundances. The resulting ~3He production rates in olivine at sea level at 29°latitude are 82±14 and 82±8 atoms g~(-1) a~(-1), as obtained from the 152 ka and 281 ka old flows, respectively. Considering effects of erosion on the 1.35 Ma old flow we find that the production rate of 82±8 atoms g~(-1) a~(-1) is consistent with the cossmogenic ~3He production during the last 1.35 Ma. There appears to be a 14% discrepancy between previously published production rates derived at higher latitudes and altitudes if the scaling factors of Lal are used to compare results. This discrepancy is greatly reduced, however, if the revised scaling factors of Dunai (this issue) are applied. Using the new scaling factors we derive a production rate for cosmogenic ~3He in olivine at sea level and high latitudes (>60°) of 118±11 atoms g~(-1) a~(-1) (±2σ). The correspondingly revised value of Cerling and Craig, and Ackert et al.) is 123 ± 6 atoms g~(-1) a~(-1) (±2σ). The mean value of these two calibrations is 121 ± 6 atoms g~(-1) a~(-1) (±2σ). We suggest that the production rate of 121 ± 6 atoms g~(-1) a~(-1) at sea level and high latitudes may be applied to the complete time range where paleomagnetic data indicate that there was no long-term averaged intensity variation in the Earth's magnetic field, i.e. over the last 10 Ma.
机译:最后一组1.35 Ma的时间序列显示了橄榄石的宇宙综合〜3He生产率。我们调查了来自西班牙加那利群岛兰萨罗特岛的三个玄武岩熔岩流顶,通过增量激光加热浸出的地层样品确定的玄武岩流的〜(40)Ar /〜(39)Ar年龄为152±26 ka,281±19 ka和1.35±0.01 Ma(±2σ)。从每个流中分析了三个或四个不同的橄榄石表晶样品的宇宙成因〜3He丰度。分别从152 ka和281 ka的旧流中获得的结果,在29度纬度的海平面处,橄榄石中〜3He的生产率为82±14和82±8个原子g〜(-1)a〜(-1)。 。考虑到侵蚀对1.35 Ma老流的影响,我们发现82±8原子g〜(-1)a〜(-1)的产生速率与最后1.35 Ma期间的宇宙成矿〜3He产生速率一致。如果使用Lal的比例因子比较结果,则先前发布的在较高纬度和海拔高度的生产率之间似乎存在14%的差异。但是,如果应用修订的Dunai缩放比例因子(此问题),则可以大大减少这种差异。利用新的比例因子,我们得出了在海平面和高纬度(> 60°)的橄榄石中,宇宙成因〜3He的生产率为118±11个原子g〜(-1)a〜(-1)(±2σ)。 Cerling和Craig以及Ackert等人的相应修订值是123±6原子g〜(-1)a〜(-1)(±2σ)。这两个校准的平均值为121±6个原子g〜(-1)a〜(-1)(±2σ)。我们建议在海平面和高纬度地区将121±6原子g〜(-1)a〜(-1)的生产率应用于整个时间范围,在整个时间范围内,古磁数据表明没有长期平均强度地球磁场的变化,即过去10 Ma的变化。

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