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Inclusion of the Two-Electron Terms

For many-electron systems we wish to incorporate the two-electron terms of the Hamiltonian into the model. As for the one-electron terms, we may perform an unnormalized Foldy-Wouthuysen transformation on the two-electron integrals to obtain a transformed set of integrals. [Pg.388]

Naturally, we also need a new expression for X that includes the two-electron terms, and this we get from the Dirac-Hartree-Fock equations, which we represent here in unrestricted form. [Pg.389]

The definition we end up with is recursive because both and contain X if we replace AF with XA throughout. In an iterative scheme this would not be a serious problem because we could use the value of X from the previous iteration to construct the J and K matrices, and at convergence the input and output X matrices would be the same to the required numerical precision. [Pg.389]

With the expressions for the density, the direct and the exchange matrices, and the definition of the transformed integrals, we can write down the NESC SCF equation as [Pg.390]

We have so far only considered the Coulomb interaction, but it is straightforward to incorporate the Gaunt or Breit interactions. [Pg.390]


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Two-electron terms

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