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A study of the observed shift in the peak position of olivine Raman spectra as a result of shock induced by hypervelocity impacts

机译:对超高速撞击引起的冲击导致的橄榄石拉曼光谱峰位位移的研究

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Kuebler etal. (2006) identified variations in olivine Raman spectra based on the composition of individual olivine grains, leading to identification of olivine composition from Raman spectra alone. However, shock on a crystal lattice has since been shown to result in a structural change to the original material, which produces a shift in the Raman spectra of olivine grains compared with the original unshocked olivine (Foster etal. 2013). This suggests that the use of the compositional calculations from the Raman spectra, reported in Kuebler etal. (2006), may provide an incorrect compositional value for material that has experienced shock. Here, we have investigated the effect of impact speed (and hence peak shock pressure) on the shift in the Raman spectra for San Carlos olivine (Fo(91)) impacting Al foil. Powdered San Carlos olivine (grain size 1-10m) was fired at a range of impact speeds from 0.6 to 6.1kms(-1) (peak shock pressures 5-86 GPa) at Al foil to simulate capture over a wide range of peak shock pressures. A permanent change in the Raman spectra was found to be observed only for impact speeds greater than similar to 5kms(-1). The process that causes the shift is most likely linked to an increase in the peak pressure produced by the impact, but only after a minimum shock pressure associated with the speed at which the effect is first observed (here 65-86 GPa). At speeds around 6kms(-1) (peak shock pressures similar to 86 GPa), the shift in Raman peak positions is in a similar direction (red shift) to that observed by Foster etal. (2013) but of twice the magnitude.
机译:Kuebler等。 (2006年)基于单个橄榄石晶粒的成分确定了橄榄石拉曼光谱的变化,从而仅从拉曼光谱中鉴定出橄榄石成分。然而,自那时起,晶格受到的冲击已导致原始材料发生结构变化,与原始未震动的橄榄石相比,橄榄石晶粒的拉曼光谱发生了位移(Foster等人,2013)。这表明使用了Kuebler等人报道的拉曼光谱中的成分计算。 (2006年),可能会给遭受冲击的材料提供不正确的成分值。在这里,我们已经研究了撞击速度(以及峰值冲击压力)对San Carlos橄榄石(Fo(91))撞击铝箔的拉曼光谱变化的影响。在铝箔上以0.6至6.1kms(-1)的冲击速度(峰值冲击压力为5-86 GPa)发射粉末状的San Carlos橄榄石(粒度1-10m),以模拟在宽范围的峰值冲击下的捕获压力。发现仅在大于5kms(-1)的撞击速度下才能观察到拉曼光谱的永久变化。引起位移的过程最有可能与冲击产生的峰值压力增加有关,但只有在与首次观察到作用的速度(此处为65-86 GPa)相关的最小冲击压力之后。在大约6kms(-1)的速度(峰值冲击压力类似于86 GPa)下,拉曼峰位置的位移与Foster等人观察到的方向相似(红色位移)。 (2013年),但幅度是其两倍。

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