Based on an exact functional form derived for the three-point vertex function , we propose a self-consistent calculation scheme for the electron self-energy with always satisfying the Ward identity. This scheme is basically equivalent to the one proposed in 2001, but it is improved in the aspects of computational costs and its applicability range; it can treat a low-density electron system with a dielectric catastrophe. If it is applied to semiconductors and insulators, we find that the obtained quasiparticle dispersion is virtually the same as that in the one-shot approximation (or A), indicating that the A actually takes proper account of both vertex and high-order self-energy corrections in a mutually cancelling manner.

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