Levels in ^(13)N Examined by ^(12)C+p Resonance Elastic Scattering via Thick Target Method  

Levels in ^(13)N Examined by ^(12)C+p Resonance Elastic Scattering via Thick Target Method

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作  者:QIN Xing WANG You-bao WANG Bao-xiang BAI Xi-xiang GUO Bing JIANG Chao LI Yun-ju LI Zhi-hong LIAN Gang SU Jun ZENG Sheng LIU Wei-ping 

机构地区:[1]Institute of Modern Physics, Shanxi Normal University, China [2]Institute of Physical Engineering, Zhengzhou University, China [3]不详

出  处:《Annual Report of China Institute of Atomic Energy》2007年第1期113-114,共2页中国原子能科学研究院年报(英文版)

基  金:National Natural Science Foundation of China (10445004, 10575136) ;Major State Basic Research Development Program (G2007CB815003)

摘  要:The conventional proton resonance scattering has been a powerful spectroscopic tool to explore the properties of compound nucleus levels close to the threshold, which is usually of astrophysicalThe conventional proton resonance scattering has been a powerful spectroscopic tool to explore the properties of compound nucleus levels close to the threshold, which is usually of astrophysical and structural significance. It is a kind of precise yet very time-consuming experiment, since one needs to change the proton beam energy in small steps in order to obtain an excitation function of the energy range of interest. To use radioactive ion beams with limited intensity and short lifetime, more efficient experimental method with the emphasis of inverse kinematics must be employed. For this purpose, the thick target method has been proposed and rapidly applied. It uses an either solid or gas target containing hydrogen atoms with thickness enough to stop the beam ions or degrade its energy to the region of interest. By measuring the lighter recoil particles at laboratory forward angles, one can rebuild the reaction kinematics taking account of the energy losses of particles in the target. The method allows one to study several resonances simultaneously by using a single bombarding energy of exotic beam.

关 键 词:核子物理学 弹性共振散射 厚目标法   质子共振散射 

分 类 号:O571[理学—粒子物理与原子核物理]

 

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