Continuity equation and local gauge invariance for the N3LO nuclear energy density functionals

被引:17
|
作者
Raimondi, F. [1 ]
Carlsson, B. G. [2 ]
Dobaczewski, J. [1 ,3 ]
Toivanen, J. [1 ]
机构
[1] Univ Jyvaskyla, Dept Phys, FI-40014 Jyvaskyla, Finland
[2] Lund Univ, Dept Math Phys, LTH, SE-22100 Lund, Sweden
[3] Univ Warsaw, Fac Phys, Inst Theoret Phys, PL-00681 Warsaw, Poland
来源
PHYSICAL REVIEW C | 2011年 / 84卷 / 06期
基金
芬兰科学院;
关键词
MATRIX EXPANSION; MEAN-FIELD;
D O I
10.1103/PhysRevC.84.064303
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
Background: The next-to-next-to-next-to-leading order ((NLO)-L-3) nuclear energy density functional extends the standard Skyrme functional with new terms depending on higher-order derivatives of densities, introduced to gain better precision in the nuclear many-body calculations. A thorough study of the transformation properties of the functional with respect to different symmetries is required as a step preliminary to the adjustment of the coupling constants. Purpose: We determine to what extent the presence of higher-order derivatives in the functional can be compatible with the continuity equation. In particular, we study the relations between the validity of the continuity equation and the invariance of the functional under gauge transformations. Methods: We derive conditions for the validity of the continuity equation in the framework of time-dependent density functional theory. The conditions apply separately to the four spin-isospin channels of the one-body density matrix. Results: We obtained four sets of constraints on the coupling constants of the (NLO)-L-3 energy density functional that guarantee the validity of the continuity equation in all spin-isospin channels. In particular, for the scalar-isoscalar channel, the constraints are the same as those resulting from imposing the standard U(1) local-gauge-invariance conditions. Conclusions: The validity of the continuity equation in the four spin-isospin channels is equivalent to the local-gauge invariance of the energy density functional. For vector and isovector channels, such validity requires the invariance of the functional under local rotations in the spin and isospin spaces.
引用
收藏
页数:11
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