Optical model potentials for deuteron scattering off $^{24}$Mg, $^{28}$Si, $^{58}$Ni, $^{90}$Zr, $^{116}$Sn, and $^{208}$Pb at $\sim$100 MeV/nucleon

D. Patel, D. C. Cuong, K. B. Howard, U. Garg, Dao T. Khoa, H. Akimune, G. P. A. Berg, M. Fujiwara, M. N. Harakeh, M. Itoh, C. Iwamoto, T. Kawabata, K. Kawase, J. T. Matta, T. Murakami, M. Yosoi
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Abstract

Angular distributions of the elastic and inelastic deuteron-nucleus scattering off $^{24}$Mg, $^{28}$Si, $^{58}$Ni, $^{90}$Zr, $^{116}$Sn, and $^{208}$Pb have been measured at a beam energy of 98 MeV/nucleon, with the goal of constraining the deuteron optical potential in this kinematical regime, and to extract the reduced transition probabilities for the ground-state transitions to low-lying excited states of these nuclei. Two potential models were used in the analysis of the measured $(d,d)$ and $(d,d')$ data within the optical model and the distorted-wave Born approximation: the phenomenological optical model potential associated with the collective model of nuclear scattering, and the semi-microscopic double-folding model of the deuteron-nucleus potential based on a realistic density-dependent M3Y interaction. The deuteron optical potential and inelastic $(d,d')$ scattering form factors were calculated using these two potential models, allowing for a direct comparison between the potential models as well as the validation of the deduced $E\lambda$ transition rates.
氘核在 $^{24}$Mg, $^{28}$Si, $^{58}$Ni, $^{90}$Zr, $^{116}$Sn 和 $^{208}$Pb 以 $\sim$100 MeV/nucleon 发生散射时的光学模型电位
在 98 MeV/核子的束流能量下,测量了^{24}$Mg、^{28}$Si、^{58}$Ni、^{90}$Zr、^{116}$Sn 和^{208}$Pb 的弹性和非弹性氘核散射的角度分布、目的是对这一运动机制中的氘核光学势进行约束,并提取这些原子核从基态过渡到低洼激发态的还原过渡概率。在分析光学模型和畸变波玻恩近似中的$(d,d)$ 和$(d,d')$ 测量数据时使用了两种电势模型:与核散射集体模型相关的现象学光学模型电势,以及基于现实密度依赖的 M3Y 作用的氘核电势半微观双折叠模型。利用这两种势模型计算了氘核光学势和非弹性 $(d,d')$ 散射形式因子,从而可以直接比较势模型之间的差异,并验证所诱导的 $E\lambda$ 转换率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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