Scalar Nature of the Nuclear Density Functional
arXiv:0801.3447 · doi:10.1103/PhysRevC.78.014307
Abstract
Because of the rotational invariance of the nuclear Hamiltonian, there exists a density functional for nuclei that depends only on two scalar densities. Practical calculations boil down to radial, one-dimensional ones.
4 pages
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- A Minimal Nuclear Energy Density Functional
- Density functional approaches to collective phenomena in nuclei: Time-dependent density-functional theory for perturbative and non-perturbative nuclear dynamics
- Density functional theory and Kohn-Sham scheme for self-bound systems
- Effective density functionals beyond mean field
- Turning the nuclear energy density functional method into a proper effective field theory: reflections
- Generalization of internal Density Functional Theory and Kohn-Sham scheme to multicomponent systems, and link with traditional DFT
- The Long Journey from Ab Initio Calculations to Density Functional Theory for Nuclear Large Amplitude Collective Motion
- Density Functional Theory with Spatial-Symmetry Breaking and Configuration Mixing
- Addressing energy density functionals in the language of path-integrals I: Comparative study of diagrammatic techniques applied to the (0+0)-D -symmetric -theory
- Density functional approaches to atomic nuclei
- Density functional approaches to nuclear dynamics
- Open problems in nuclear density functional theory
- Algebraic Density Functionals
- A Many-Body Density Energy Functional
- Schrödinger equations for the square root density of an eigenmixture and % the square root of an eigendensity spin matrix