α+28Si弹性散射系统的双折叠分析

Ahmed Hammad Amer
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引用次数: 0

摘要

利用双折叠模型(DFM),我们重新分析了弹性散射[公式:见文]+[公式:见文]Si体系在[公式:见文]宽能量范围内的20组实验角分布——粒子从12.7[公式:见文]MeV到240[公式:见文]MeV。我们使用三种有效的核子-核子(NN)相互作用CDM3Y6、圣保罗势(SPP2)和巴西核势(BNP)来产生DF势。数据分析采用半显微(SM)和全显微(FM)方法进行。在SM方法中,使用DFM创建光势(OP)的实部,并考虑了OP的虚部的Woods-Saxon (WS)势。在FM方法中,提取了OP的实部和虚部的DF势重整化因子[公式:见文]和[公式:见文]。我们研究了[公式:见文]和[公式:见文]因子的能量依赖性,以及核势体积积分和反应截面的能量依赖性。我们使用[公式:见文]和[公式:见文]从它们的能量依赖函数中获得的因子合理地再现了数据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Double Folding Analysis of the α+28Si Elastic Scattering System
Using the double folding model (DFM), we reanalyzed 20 sets of experimental angular distributions for the elastic scattering [Formula: see text]+[Formula: see text]Si system in a wide energy range of [Formula: see text]-particles from 12.7[Formula: see text]MeV to 240[Formula: see text]MeV. We used three effective nucleon–nucleon (NN) interactions that are CDM3Y6, São Paulo Potential (SPP2), and Brazilian Nuclear Potential (BNP) to generate the DF potentials. The data analysis was performed using semi-microscopic (SM) and fully microscopic (FM) methods. In the SM approach, the real part of the optical potential (OP) is created with the DFM, and the Woods–Saxon (WS) potential is considered for the imaginary part of the OP. In the FM approach, the DF potential renormalization factors [Formula: see text] and [Formula: see text] for the real and imaginary parts of the OP were extracted. We investigated the energy dependencies of the [Formula: see text] and [Formula: see text] factors, as well as of nuclear potential volume integrals and reaction cross-sections. We reasonably reproduced the data using [Formula: see text] and [Formula: see text] factors obtained from their energy-dependent functions.
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