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超重核的壳结构
引用本文:张炜,孟杰,张双全,耿立升,H.Toki. 超重核的壳结构[J]. 原子核物理评论, 2004, 21(4): 368-369. DOI: 10.11804/NuclPhysRev.21.04.368
作者姓名:张炜  孟杰  张双全  耿立升  H.Toki
作者单位:1 兰州重离子加速器国家实验室原子核理论中心;甘肃兰州7300002 北京大学物理学院; 北京1008713 中国科学院理论物理研究所 北京100080;4 Research Center for Nuclear Physics (RCNP); Osaka University; Ibaraki; Osaka; 567-0047; Japan
基金项目:国家重点基础研究发展规划资助项目(G2000077407),国家自然科学基金资助项目(10025522,10221003,10047001)~~
摘    要:在相对论连续谱Hartree Bogoliubov(RCHB)理论框架下,在质子数Z=100—140和中子数N=Z+30—2Z+32等偶偶核中进行了超重球形双幻核的探索.采用的有效相互作用为NL1,NL3,NLSH,TM1,TW 99,DD ME1,PK1和PK1R.基于对双核子分离能(S2p和S2n)、双核子能隙(δ2p和δ2n)、壳修正能量(Epshell)、对能(Eppair和Enpair)和有效对能隙(Δp和Δn)等物理量和能shell和En级结构的分析,预言了可能的质子幻数和中子幻数,并观察到在超重核区壳的弱化现象. The magic proton and neutron numbers are searched in the superheavy region with proton number Z=100 —140 and neutron number N=(Z+30) — (2Z+32) by the relativistic continuum Hartree-Bogoliubov (RCHB) theory with interactions NL1, NL3, NLSH, TM1, TW99, DD-ME1, PK1, and PK1R. Based on the two-nucleon separation energies S_(2p )and S_(2n) , the two-nucleon gaps δ_(2p) and δ_(2n), the shell correction energies E~p_(shell) and E~n_(shell), the pairing energies E~p_(pair) and E~n_(pair), and...

关 键 词:超重核   相对论平均场理论   壳结构
文章编号:1007-4627(2004)04-0368-03
收稿时间:1900-01-01

Shell Structure of Superheavy Nuclei
ZHANG Wei. Shell Structure of Superheavy Nuclei[J]. Nuclear Physics Review, 2004, 21(4): 368-369. DOI: 10.11804/NuclPhysRev.21.04.368
Authors:ZHANG Wei
Affiliation:(1 Center of Theoretical Nuclear Physics; National Laboratory of Heavy Ion Accelerator of Lanzhou; Lanzhou 730000; China; 2 School of Physics; Peking University; Beijing 100871; 3 Institute of Theoretical Physics; Chinese Academy of Sciences; Beijing 100080; 4 Research Center for Nuclear Physics (RCNP); Osaka University; Ibaraki; Osaka; 567-0047; Japan);
Abstract:The magic proton and neutron numbers are searched in the superheavy region with proton number Z=100 —140 and neutron number N=(Z+30) — (2Z+32) by the relativistic continuum Hartree-Bogoliubov (RCHB) theory with interactions NL1, NL3, NLSH, TM1, TW99, DD-ME1, PK1, and PK1R. Based on the two-nucleon separation energies S_(2p )and S_(2n) , the two-nucleon gaps δ_(2p) and δ_(2n), the shell correction energies E~p_(shell) and E~n_(shell), the pairing energies E~p_(pair) and E~n_(pair), and...
Keywords:superheavy nuclei  relativistic mean field theory  shell structure
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