Total energy is obtained from the Kohn-Sham equations via an integral over electron density and orbitals.
the verdict
CONTESTED
contested - the weight sits with the supporting side
refutedsupported
the weight of evidence
2 sources for · 0 against
The available sources mention universal functionals of the density and molecular orbitals in quantum chemistry, but do not fully establish that total energy is obtained via an integral over electron density and orbitals through the Kohn-Sham equations.
For obtaining individual excited-state energies and densities of Coulomb electronic systems, by means of an energy stationary principle, it was shown previously that there exists a universal functional of the density, FCoul[ϱ], for the kinetic plus electron-electron repulsion part of the total energy. Here, we make knowledge of the existence of FCoul[ϱ] practical for calculation by identifying TsCoul[ϱ], the non-interacting kinetic energy component of FCoul[ϱ], and by showing that TsCoul[ϱ] may be computed exactly by means of orbitals that are obtained through a set of single-particle Kohn-Sham equations. Constraints for obtaining accurate approximations to the remaining unknown component of FCoul[ϱ] are presented.
filled with electrons from two different atomic orbitals. These atomic orbitals come from separate atoms resulting in molecular orbitals being linear
Quantum chemistry, or molecular quantum mechanics, is a branch of physical chemistry which applies quantum mechanics to chemical systems to predict physical and chemical properties of molecules and materials. Calculations, which involve calculating electronic wave functions at the atomic level, make approximations to make simulations computationally feasible while capturing the relevant contribut
The Thomas–Fermi model was developed independently by Thomas and Fermi in 1927. This was the first attempt to describe many-electron systems on the basis of electronic density instead of wave functions, although it was not very successful in the treatment of entire molecules. The method did provide the basis for what is now known as density functional theory (DFT). Modern day DFT uses the Kohn–Sham method, where the density functional is split into four terms; the Kohn–Sham kinetic energy, an external potential, exchange and correlation energies. A large part of the focus on developing DFT is on improving the exchange and correlation terms. Though this method is less developed than post Hartree–Fock methods, its significantly lower computational requirements (scaling typically no worse than n3 with respect to n basis functions, for the pure functionals) allow it to tackle larger polyatomic molecules and even macromolecules. This computational affordability and often comparable accuracy to MP2 and CCSD(T)…
Everything we examined (2)
This check searched the claim as stated. It did not run a separate search for evidence against it.