摘要
作者在9°~130°散射角范围,测量了22MeV质子在12C,13C上的弹性散射微分截面以及在13C核1/2+(3.09MeV),3/2-(3.68MeV)和5/2+(3.85MeV)激发态上的非弹性散射微分截面.对12C,13C弹性散射微分截面进行了微观光学势分析,计算结果能较好地描述实验数据.采用全微观扭曲波玻恩近似(DWBA)理论对非弹性散射实验数据进行了分析.通过小角区实验数据与理论计算结果的比较,进一步证实了13C的1/2+(3.09MeV)激发态存在中子晕结构.根据13C核1/2+(3.09MeV)激发态的其它实验结果,对1/2+(3.09MeV)态的壳模型单体密度矩阵元(OBDME)进行了修正.修正后的壳模型OBDME能较好地描述从电子散射实验得到的1/2+(3.09MeV)态的纵向和横向形状因子(formfactor)以及547MeV质子非弹性散射微分截面.另外,作者在1/2+(3.09MeV)态的质子非弹性散射实验中观察到微分截面位于120°附近的一个宽峰,该峰可能与核的π场效应(pionfieldeffect)有关.全微观DWBA计算结果大体上能给出3/2-(3.68MeV)和5/2+(3.85MeV)激发态实验数据的幅度大小,但对细节的描述还不能令人满意.作者的研究还表明了对13C核作仔细的大规模壳模型计算以及基于现代核子 核子力构造低能区密度依赖的完整的有效相互作用的必要性.
The differential cross sections of 22 MeV proton elastic scattering from 12C,13C nuclei and inelastic scattering for 1/2+(3.09MeV), 3/2-(3.68MeV) and 5/2+(3.85MeV) excitation states of 13C nucleus have been measured between 9° and 130°. The measured elastic scattering data have been compared with the results of microscopic optical potential based upon the effective nn interaction (CEG). Good agreement is obtained. The broad peak located at about 120° for 13C 1/2+(3.09MeV) state has been observed for the first time in the present proton inelastic scattering. The present experimental data for inelastic scattering were analyzed by using full microscopic distortedwave Born approximation (DWBA). From the comparison of present experimental data and theoretical results at forward angles, the authors' analysis indicates the existence of neutron halo in the 13C 1/2+(3.09MeV) excitation state. In addition, by reasonable modification of shell model wavefunction of 13C 1/2+(3.09MeV) excitation state, we can better describe the experimental form factors of (e,e′) and the experimental differential cross sections of (p,p′) at incident energy of 547 MeV. For the 13C 3/2-(3.68MeV) and 5/2+(3.85MeV) states, the full microscopic DWBA analyses can only provide a general description to the experimental data.
出处
《四川大学学报(自然科学版)》
CAS
CSCD
北大核心
2003年第5期905-911,共7页
Journal of Sichuan University(Natural Science Edition)
基金
国家自然科学基金(19975032)