Abstract
A method is described for the complete calculation of electronic energies in crystalline solids without approximating overlap, electron-repulsion, or exchange contributions. The practicality of the method is confirmed by preliminary results, which also indicate reasons for the considerable success of independent-electron methods.
- Received 4 August 1969
DOI:https://doi.org/10.1103/PhysRevLett.23.1026
©1969 American Physical Society