2002
DOI: 10.1002/qua.940
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Quantum electrodynamical density‐matrix functional theory and group theoretical consideration of its solution

Abstract: ABSTRACT:For studying the group theoretical classification of the solutions of the density functional theory in relativistic framework, we propose quantum electrodynamical density-matrix functional theory (QED-DMFT). QED-DMFT gives the energy as a functional of a local one-body 4 × 4 matrix Q(x) ≡ − ψ(x)ψ(x) , where ψ andψ are a 4-component Dirac field and its Dirac conjugate, respectively. We examine some characters of QED-DMFT. After these preparations, by using Q(x), we classify the solutions of QED-DMFT un… Show more

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Cited by 7 publications
(7 citation statements)
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“…The computational scheme is illustrated in Figure 6. We already discussed similar strategies in the case of spin‐free Hamiltonian 21 and QED Hamiltonian 22.…”
Section: Resultsmentioning
confidence: 99%
“…The computational scheme is illustrated in Figure 6. We already discussed similar strategies in the case of spin‐free Hamiltonian 21 and QED Hamiltonian 22.…”
Section: Resultsmentioning
confidence: 99%
“…Even more generally, one could consider functionals of the local density matrix n( r) = 〈Ψ|n( r)|Ψ〉, as proposed in Ref. [13]. For simplicity, in the following, the opposite charge density and opposite charge current will be referred to as charge density and charge current.…”
Section: Density-functional Theory Based On Effective Quantum Electrodynamicsmentioning
confidence: 99%
“…Eschrig et al [11,12] took another approach to RDFT based on Lieb's Legendre transformation using a normalordered QED Hamiltonian. Ohsaku et al [13] proposed a local-density-matrix functional theory based on a QED Hamiltonian with an one-photon-propagator fermion-fermion interaction. Despite these formal foundations of RDFT based on QED, in practice four-component RDFT is invariably applied in the Kohn-Sham (KS) scheme with a non-quantized electromagnetic field and in the no-pair approximation (i.e., neglecting contributions from electron-positron pairs) [14][15][16][17][18][19][20][21], most of the time using non-relativistic exchange-correlation density functionals.…”
Section: Introductionmentioning
confidence: 99%
“…* marm3. 14@gmail.com Already in 2002 Ohsaku et al introduced a local (relativistic) quantum electro-dynamical (QED) RDMFT [40] theory in which the nonlocality properties of the firstorder reduced density matrix (1-RDM) were not exploited and the so-called noninteracting kinetic energy needed to be evaluated with an auxiliary noninteracting system. This complication may be avoided by using the full 1-RDM as all one-body interactions can then be evaluated as explicitly known functionals of the 1-RDM.…”
Section: Introductionmentioning
confidence: 99%