290AMeV时元素目标上的碳碎片

Hailong Duan, Jing-Ya Wu, T. Ma, Jun-Sheng Li, Hui-Ling Li, Ming-ming Xu, Ruizhu Yang, Dong-Hai Zhang, Zhi Zhang, Qi Wang, S. Kodaira
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引用次数: 1

摘要

研究了12C在最高能量为290 MeV的C、Al、Cu、Pb和CH2靶上破碎产生抛射破片的总变电荷截面和部分破片截面。结果表明,PFs的总变电荷反应截面和部分变电荷反应截面与束流能量无关,在相同束流能量下,随目标质量的增加而增大。总变电荷反应截面与Bradt-Peters半经验公式、PHITS和NUCFRG2模拟模型的预测结果一致。随着目标质量的增加,PFs生成的部分截面增大,这与NUCFRG2模型的预测结果一致。弹丸颗粒的平均散射角小于PF的平均发射角,弹丸颗粒的散射角分布宽度小于PF的发射角分布宽度。在我们所研究的束流能区,光子激光器的平均发射角与目标质量和束流能量没有明显的关系。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Fragmentation of carbon on elemental targets at 290AMeV
The total charge-changing cross-sections and the partial cross-sections for projectile fragments (PFs) production for the fragmentation of 12C on C, Al, Cu, Pb and CH2 targets at the highest energy of 290[Formula: see text]A[Formula: see text]MeV were studied. It was found that the total charge-changing reaction cross-sections and the partial reaction cross-sections of PFs production were independent of the beam energy, and increased with increase of mass of target for the same beam energy. The total charge-changing reaction cross-section was the same as the prediction of Bradt–Peters semi-empirical formula, PHITS and NUCFRG2 simulation models. The partial cross-section of PFs production increased with the increase of the mass of target, and it was the same as the prediction of NUCFRG2 models. The mean scattering angle of projectile particle was smaller than the average emission angle of PF, and the width of scattering angle distribution of projectile particle was smaller than that of emission angle distribution of PFs. The mean emission angle of PFs does not obviously depend on the target mass and beam energy in our studied beam energy regions.
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