Читать книгу Quantum Mechanics, Volume 3 - Claude Cohen-Tannoudji - Страница 149

Let us return to the particular case of fermions all having the same spin state, as in § 1 of Complement E_XV. We can then write the Hartree-Fock equations in terms of the wave functions as:

(37)

using definitions of (46) of that complement for the direct and exchange potentials, which are now time-dependent. There is obviously a close relation between the Hartree-Fock equations, whether they are time-dependent or not.