6Li+28Si弹性散射的不同折叠模型

A. Ibraheem, M. Farid, E. A. El-Rahman, Z. Mahmoud, S. R. Mokhtar
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摘要

本文分析了6Li+[公式:见文]Si体系在76 ~ 318 MeV宽能量范围内的弹性散射。在光学模型(OM)的框架下进行分析。采用了两种不同的方法来计算该系统的核光势。第一种方法是用Woods-Saxon (WS)形式对虚部提供实部的双折叠聚类(DFC)。在第二种方法中,使用基于圣保罗势(SPP)的双折叠(DF)模型作为实部和虚部,各乘以相应的归一化因子。对于[公式:见文]Si,考虑完整的[公式:见文]-簇密度,而对于6Li,考虑[公式:见文]-氘核([公式:见文]-[公式:见文])结构。因此,DFC实中心部分是通过折叠[公式:见文]-[公式:见文]和[公式:见文]-[公式:见文]靶核之间的有效相互作用超过靶弹的簇密度来计算的。导出的重归一化电位成功地描述了数据。本文的结果与前人的工作很好地吻合。这种一致性证实了本方法产生核-核光势的有效性。
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Different folding models for 6Li+28Si elastic scattering
In this work, the elastic scattering of 6Li+[Formula: see text]Si system at wide range energies from 76 to 318[Formula: see text]MeV is analyzed. The analysis is carried out in the framework of the optical model (OM). Two different methods are adopted for nuclear optical potential of this system. The first method is the double folding cluster (DFC) for the real part supplied with an imaginary part in the Woods–Saxon (WS) form. In the second one, the double folding (DF) model based upon São Paulo potential (SPP) is used as real and imaginary parts each multiplied by a corresponding normalization factor. For [Formula: see text]Si, the full [Formula: see text]-cluster density is considered while the [Formula: see text]-deuteron ([Formula: see text]–[Formula: see text]) structure is considered for 6Li. Therefore, the DFC real central part is calculated by folding both [Formula: see text]–[Formula: see text] and [Formula: see text]–[Formula: see text] effective interaction between target and nuclei over the cluster densities of the target and projectile. The derived renormalized potentials give a successful description of the data. The present results are in good agreement with the previous work. This agreement confirms the validity of the present methods to generate nucleus–nucleus optical potentials.
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