Nonlocal energy density functionals for pairing and beyond-mean-field calculations

被引:24
|
作者
Bennaceur, K. [1 ,2 ,3 ]
Idini, A. [2 ,4 ]
Dobaczewski, J. [2 ,3 ,5 ,6 ]
Dobaczewski, P. [7 ]
Kortelainen, M. [2 ,3 ]
Raimondi, F. [2 ,4 ]
机构
[1] Univ Lyon 1, Univ Lyon, CNRS, IN2P3,IPNL, F-69622 Villeurbanne, France
[2] Univ Jyvaskyla, Dept Phys, POB 35 YFL, FI-40014 Jyvaskyla, Finland
[3] Univ Helsinki, Helsinki Inst Phys, POB 64, FIN-00014 Helsinki, Finland
[4] Univ Surrey, Dept Phys, Guildford GU2 7XH, Surrey, England
[5] Univ York, Dept Phys, York YO10 5DD, North Yorkshire, England
[6] Warsaw Univ, Fac Phys, Inst Theoret Phys, Ul Pasteura 5, PL-02093 Warsaw, Poland
[7] ul Obozowa 85 m 5, PL-01425 Warsaw, Poland
基金
芬兰科学院;
关键词
energy density functionals; regularized pseudopotentials; nuclear pairing; EQUATION; NUCLEI; FORCES;
D O I
10.1088/1361-6471/aa5fd7
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
We propose to use two-body regularized finite-range pseudopotential to generate nuclear energy density functional (EDF) in both particle-hole and particle-particle channels, which makes it free from self-interaction and selfpairing, and also free from singularities when used beyond mean field. We derive a sequence of pseudopotentials regularized up to next-to-leading order and next-to-next-to-leading order, which fairly well describe infinite-nuclearmatter properties and finite open-shell paired and/or deformed nuclei. Since pure two-body pseudopotentials cannot generate sufficiently large effective mass, the obtained solutions constitute a preliminary step towards future implementations, which will include, e.g., EDF terms generated by three-body pseudopotentials.
引用
收藏
页数:22
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