We introduce an alternative route to quasiparticle self-consistent calculations () on the basis of a Joint Approximate Diagonalization of the one-body Green’s functions taken at the input quasiparticle energies. Such an approach allows working with the full dynamical self-energy, without approximating the latter by a symmetrized static form as in the standard scheme. Calculations on the 100 molecular test set lead nevertheless to a good agreement, at the 65 meV mean-absolute-error accuracy on the ionization potential, with respect to the conventional approach. We show further that constructing the density matrix from the full Green’s function as in the fully self-consistent scheme, and not from the occupied quasiparticle one-body orbitals, allows obtaining a scheme intermediate between and approaches, closer to CCSD(T) reference values.

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