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Reflection Asymmetric Relativistic Mean Field Approach and Its Application to the Octupole Deformed Nucleus ^226Ra
作者姓名:耿立升  孟杰  Toki  Hiroshi
作者单位:[1]School of Physics, Peking University, Belting 100871 [2]Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100080 [3]Center of Theoretical Nuclear Physics, National Laboratory of Heavy Ion Accelerator, Lanzhou 730000 [4]Research Center for Nuclear Physics (RCNP), Osaka University, Ibaraki 567-0047, Japan
基金项目:Supported by the National Natural Science Foundation of China under Grant Nos 10435010 and 10221003, and the Doctoral Foundation from the Ministry of Education of China.
摘    要:A reflection asymmetric relativistic mean field (RAS-RMF) approach is developed by expanding the equations of motion for both the nucleons and the mesons on the eigenfunctions of the two-centre harmonic-oscillator potential. The efficiency and reliability of the RAS-RMF approach are demonstrated in its application to the well-known octupole deformed nucleus 226Ra and the available data, including the binding energy and the deformation parameters, are well reproduced.

关 键 词:相对论  反射  八极装置  原子核
收稿时间:2007-3-20
修稿时间:2007-03-20

Reflection Asymmetric Relativistic Mean Field Approach and Its Application to the Octupole Deformed Nucleus 226Ra
GENG Li-Sheng,MENG Jie,Toki Hiroshi.Reflection Asymmetric Relativistic Mean Field Approach and Its Application to the Octupole Deformed Nucleus ^226Ra[J].Chinese Physics Letters,2007,24(7):1865-1868.
Authors:GENG Li-Sheng  MENG Jie  Toki Hiroshi
Abstract:A reflection asymmetric relativistic mean field (RAS-RMF) approach is developed by expanding the equations of motion for both the nucleons andthe mesons on the eigenfunctions of the two-centre harmonic-oscillatorpotential. The efficiency and reliability of the RAS-RMF approach are demonstrated in its application to the well-known octupole deformednucleus 226Ra and the available data, including the binding energy and the deformation parameters, are well reproduced.
Keywords:21  60  -n  21  60  Jz  21  10  Ft  21  10  Gv
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