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Energy loss and energy straggling of light ions in fullerite

机译:富勒石中轻离子的能量损失和能量散逸

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To determinate the stopping cross section in fullerite a feasible approach, taking into account the high radiation sensitivity and mechanical Fragility of Fullerite films, should be employed. In this work, the stopping cross sections of H-1, H-3, He-4 and Li-7 ions for several selected energies were measured by Rutherford backscattering, neutron depth profiling and alpha spectroscopy using sandwich structures of samples composed of fullerite deposited on a firm substrate (Si, steel) with an intermediate marker (Au, N, Li, B, Pu). In addition, ion transmission through a thin C film supporting a fullerite layer was also utilized. The measured stopping cross sections follow the theoretical predictions calculated for carbon, but are systematically (10-35%) higher than the theoretical ones (with the exception of 5 - 5.5 MeV He-4). The observed deviation of the experimental data can partly be explained by the chemical state effects in fullerite, which accounts for about 20-50% of the difference. The measured energy straggling exceeds Bohr's value by a Factor of about 2 for alpha spectroscopy and ion transmission, and 2.5 or 9.5 for Rutherford backscattering and neutron depth profiling, respectively. The discrepancy can be explained by a thickness variation, such as surface roughness of the fullerite films. [References: 23]
机译:为了确定富勒岩的截面积,应考虑富勒石薄膜的高辐射敏感性和机械脆性,采用可行的方法。在这项工作中,通过使用富勒石沉积的样品的夹心结构,通过卢瑟福反向散射,中子深度分析和α光谱测量了几种选定能量的H-1,H-3,He-4和Li-7离子的终止截面在带有中间标记(Au,N,Li,B,Pu)的坚固基材(硅,钢)上。另外,还利用了通过支持富勒石层的C薄膜的离子传输。测得的截面积符合碳的理论预测值,但系统上比理论值高(10-35%)(5-5.5 MeV He-4除外)。观察到的实验数据偏差可以部分由富勒石的化学状态效应解释,这大约占差异的20-50%。对于阿尔法光谱和离子传输,所测得的能量散布超过玻尔值的系数约为2,而对于卢瑟福背散射和中子深度分布,分别为约2或9.5的系数。差异可以通过厚度变化来解释,例如富勒岩膜的表面粗糙度。 [参考:23]

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