Resolve the low-occupation limit of the quasiparticle-weight parametrization
Develop a more careful parametrization of the quasiparticle weight for the Bethe-lattice Hubbard model in the low-occupation limit n0 so that the i-DFT exchange-correlation bias parameters, particularly 2, vanish appropriately and the resulting spectral function converges to the non-interacting Kohn-Sham spectral function.
References
In the limit of low occupation, n\to0, the spectral function does not converge to the non-interacting (i.e. the KS) spectral function given by Eq.~(\ref{sf}). Most likely, this is due to our parametrization of the quasiparticle weight not approaching unity fast enough in the limit n\to0. Hence Z{-2}-1 in the numerator of Eq.~(\ref{lambda2}) does not vanish fast enough in the limit n\to0 to compensate both for A_s(0)4 in the denominator going to zero extremely fast as well as for the divergence of A_s\prime(0) in the same limit. This prevents \lambda_2 from vanishing in this limit, as it should. We suspect that the problem can be fixed by a more careful parametrization of Z in this limit.