The kinetic energy density in Kohn-Sham density functional theory

被引:29
作者
Bhattacharyya, A [1 ]
Furnstahl, RJ [1 ]
机构
[1] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
基金
美国国家科学基金会;
关键词
density functional theory; effective field theory; effective action; skyrme functional;
D O I
10.1016/j.nuclphysa.2004.10.008
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
This work continues a program to systematically generalize the Skyrme Hartree-Fock method for medium and heavy nuclei by applying effective field theory (EFT) methods to Kohn-Sham density functional theory (DFT). When conventional Kohn-Sham DFT for Coulomb systems is extended beyond the local density approximation, the kinetic energy density tau is sometimes included in energy functionals in addition to the fermion density. However, a local (semi-classical) expansion of tau is used to write the energy as a functional of the density alone, in contrast to the Skyrme approach. The difference is manifested in different single-particle equations, which in the Skyrme case include a spatially varying effective mass. Here we show how to generalize the EFT framework for DFT derived previously to reconcile these approaches. A dilute gas of fermions with short-range interactions confined by an external potential serves as a model system for comparisons and for testing power-counting estimates of new contributions to the energy functional. (C) 2004 Elsevier B.V. All rights reserved.
引用
收藏
页码:268 / 294
页数:27
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