Exchange and correlation potential in silicon. II

Abstract
For pt.I see ibid., vol.10, p.987 (1977). A previous calculation of the exchange and correlation energy in silicon is extended to the conduction band. The authors include the self-energy operator in the electron Hamiltonian to recalculate the band structure and compare this new band structure with that from a purely local pseudopotential. A simplified method of calculating the self-energy operator is suggested.